Optical image capturing system

ABSTRACT

An optical image capturing system includes, along the optical axis in order from an object side to an image side, a first lens, a second lens, a third lens, a fourth lens, a fifth lens, a sixth lens, and a seventh lens. At least one lens among the first to the sixth lenses has positive refractive force. The seventh lens can have negative refractive force, wherein both surfaces thereof are aspheric, and at least one surface thereof has an inflection point. The lenses in the optical image capturing system which have refractive power include the first to the seventh lenses. The optical image capturing system can increase aperture value and improve the imagining quality for use in compact cameras.

The current application claims a foreign priority to application number 104131559 filed on Sep. 24, 2015 in Taiwan.

BACKGROUND OF THE INVENTION 1. Technical Field

The present invention relates generally to an optical system, and more particularly to a compact optical image capturing system for an electronic device.

2. Description of Related Art

In recent years, with the rise of portable electronic devices having camera functionalities, the demand for an optical image capturing system is raised gradually. The image sensing device of the ordinary photographing camera is commonly selected from charge coupled device (CCD) or complementary metal-oxide semiconductor sensor (CMOS Sensor). In addition, as advanced semiconductor manufacturing technology enables the minimization of the pixel size of the image sensing device, the development of the optical image capturing system towards the field of high pixels. Therefore, the requirement for high imaging quality is rapidly raised.

The conventional optical system of the portable electronic device usually has five or six lenses. However, the optical system is asked to take pictures in a dark environment, in other words, the optical system is asked to have a large aperture. The conventional optical system provides high optical performance as required.

It is an important issue to increase the quantity of light entering the lens. In addition, the modern lens is also asked to have several characters, including high image quality.

BRIEF SUMMARY OF THE INVENTION

The aspect of embodiment of the present disclosure directs to an optical image capturing system and an optical image capturing lens which use combination of refractive powers, convex and concave surfaces of seven-piece optical lenses (the convex or concave surface in the disclosure denotes the geometrical shape of an image-side surface or an object-side surface of each lens on an optical axis) to increase the quantity of incoming light of the optical image capturing system, and to improve imaging quality for image formation, so as to be applied to minimized electronic products.

The term and its definition to the lens parameter in the embodiment of the present are shown as below for further reference.

The lens parameter related to a length or a height in the lens:

A maximum height for image formation of the optical image capturing system is denoted by HOI. A height of the optical image capturing system is denoted by HOS. A distance from the object-side surface of the first lens to the image-side surface of the seventh lens is denoted by InTL. A distance from the first lens to the second lens is denoted by IN12 (instance). A central thickness of the first lens of the optical image capturing system on the optical axis is denoted by TP1 (instance).

The lens parameter related to a material in the lens:

An Abbe number of the first lens in the optical image capturing system is denoted by NA1 (instance). A refractive index of the first lens is denoted by Nd1 (instance).

The lens parameter related to a view angle in the lens:

A view angle is denoted by AF. Half of the view angle is denoted by HAF. A major light angle is denoted by MRA.

The lens parameter related to exit/entrance pupil in the lens:

An entrance pupil diameter of the optical image capturing system is denoted by HEP. For any surface of any lens, a maximum effective half diameter (EHD) is a perpendicular distance between an optical axis and a crossing point on the surface where the incident light with a maximum viewing angle of the system passing the very edge of the entrance pupil. For example, the maximum effective half diameter of the object-side surface of the first lens is denoted by EHD11, the maximum effective half diameter of the image-side surface of the first lens is denoted by EHD12, the maximum effective half diameter of the object-side surface of the second lens is denoted by EHD21, the maximum effective half diameter of the image-side surface of the second lens is denoted by EHD22, and so on.

The lens parameter related to an arc length of the shape of a surface and a surface profile:

For any surface of any lens, a profile curve length of the maximum effective half diameter is, by definition, measured from a start point where the optical axis of the belonging optical image capturing system passes through the surface of the lens, along a surface profile of the lens, and finally to an end point of the maximum effective half diameter thereof. In other words, the curve length between the aforementioned start and end points is the profile curve length of the maximum effective half diameter, which is denoted by ARS. For example, the profile curve length of the maximum effective half diameter of the object-side surface of the first lens is denoted by ARS11, the profile curve length of the maximum effective half diameter of the image-side surface of the first lens is denoted by ARS12, the profile curve length of the maximum effective half diameter of the object-side surface of the second lens is denoted by ARS21, the profile curve length of the maximum effective half diameter of the image-side surface of the second lens is denoted by ARS22, and so on.

For any surface of any lens, a profile curve length of a half of the entrance pupil diameter (HEP) is, by definition, measured from a start point where the optical axis of the belonging optical image capturing system passes through the surface of the lens, along a surface profile of the lens, and finally to a coordinate point of a perpendicular distance where is a half of the entrance pupil diameter away from the optical axis. In other words, the curve length between the aforementioned stat point and the coordinate point is the profile curve length of a half of the entrance pupil diameter (HEP), and is denoted by ARE. For example, the profile curve length of a half of the entrance pupil diameter (HEP) of the object-side surface of the first lens is denoted by ARE11, the profile curve length of a half of the entrance pupil diameter (HEP) of the image-side surface of the first lens is denoted by

ARE 12, the profile curve length of a half of the entrance pupil diameter (HEP) of the object-side surface of the second lens is denoted by ARE21, the profile curve length of a half of the entrance pupil diameter (HEP) of the image-side surface of the second lens is denoted by ARE22, and so on.

The lens parameter related to a depth of the lens shape:

A distance in parallel with the optical axis from a point where the optical axis passes through to an end point of the maximum effective semi diameter on the object-side surface of the seventh lens is denoted by InRS71 (the depth of the maximum effective semi diameter). A distance in parallel with the optical axis from a point where the optical axis passes through to an end point of the maximum effective semi diameter on the image-side surface of the seventh lens is denoted by InRS72 (the depth of the maximum effective semi diameter). The depth of the maximum effective semi diameter (sinkage) on the object-side surface or the image-side surface of any other lens is denoted in the same manner.

The lens parameter related to the lens shape:

A critical point C is a tangent point on a surface of a specific lens, and the tangent point is tangent to a plane perpendicular to the optical axis and the tangent point cannot be a crossover point on the optical axis. Following the above description, a distance perpendicular to the optical axis between a critical point C51 on the object-side surface of the fifth lens and the optical axis is HVT51 (instance), and a distance perpendicular to the optical axis between a critical point C52 on the image-side surface of the fifth lens and the optical axis is HVT52 (instance). A distance perpendicular to the optical axis between a critical point C61 on the object-side surface of the sixth lens and the optical axis is HVT61 (instance), and a distance perpendicular to the optical axis between a critical point C62 on the image-side surface of the sixth lens and the optical axis is HVT62 (instance). A distance perpendicular to the optical axis between a critical point on the object-side or image-side surface of other lenses, such as the seventh lens, and the optical axis is denoted in the same manner.

The object-side surface of the seventh lens has one inflection point IF711 which is nearest to the optical axis, and the sinkage value of the inflection point IF711 is denoted by SGI711 (instance). A distance perpendicular to the optical axis between the inflection point IF711 and the optical axis is HIF711 (instance). The image-side surface of the seventh lens has one inflection point IF721 which is nearest to the optical axis, and the sinkage value of the inflection point IF721 is denoted by SGI721 (instance). A distance perpendicular to the optical axis between the inflection point IF721 and the optical axis is HIF721 (instance).

The object-side surface of the seventh lens has one inflection point IF712 which is the second nearest to the optical axis, and the sinkage value of the inflection point IF712 is denoted by SGI712 (instance). A distance perpendicular to the optical axis between the inflection point IF712 and the optical axis is HIF712 (instance). The image-side surface of the seventh lens has one inflection point IF722 which is the second nearest to the optical axis, and the sinkage value of the inflection point IF722 is denoted by SGI722 (instance). A distance perpendicular to the optical axis between the inflection point IF722 and the optical axis is HIF722 (instance).

The object-side surface of the seventh lens has one inflection point IF713 which is the third nearest to the optical axis, and the sinkage value of the inflection point IF713 is denoted by SGI713 (instance). A distance perpendicular to the optical axis between the inflection point IF713 and the optical axis is HIF713 (instance). The image-side surface of the seventh lens has one inflection point IF723 which is the third nearest to the optical axis, and the sinkage value of the inflection point IF723 is denoted by SGI723 (instance). A distance perpendicular to the optical axis between the inflection point IF723 and the optical axis is HIF723 (instance).

The object-side surface of the seventh lens has one inflection point IF714 which is the fourth nearest to the optical axis, and the sinkage value of the inflection point IF714 is denoted by SGI714 (instance). A distance perpendicular to the optical axis between the inflection point IF714 and the optical axis is HIF714 (instance). The image-side surface of the seventh lens has one inflection point IF724 which is the fourth nearest to the optical axis, and the sinkage value of the inflection point IF724 is denoted by SGI724 (instance). A distance perpendicular to the optical axis between the inflection point IF724 and the optical axis is HIF724 (instance).

An inflection point, a distance perpendicular to the optical axis between the inflection point and the optical axis, and a sinkage value thereof on the object-side surface or image-side surface of other lenses is denoted in the same manner.

The lens parameter related to an aberration:

Optical distortion for image formation in the optical image capturing system is denoted by ODT. TV distortion for image formation in the optical image capturing system is denoted by TDT. Further, the range of the aberration offset for the view of image formation may be limited to 50%-100% field. An offset of the spherical aberration is denoted by DFS. An offset of the coma aberration is denoted by DFC.

Transverse aberration on an edge of an aperture is denoted by STA, which stands for STOP transverse aberration, and is used to evaluate the performance of one specific optical image capturing system. The transverse aberration of light in any field of view can be calculated with a tangential fan or a sagittal fan. More specifically, the transverse aberration caused when the longest operation wavelength (e.g., 650 nm) and the shortest operation wavelength (e.g., 470 nm) pass through the edge of the aperture can be used as the reference for evaluating performance. The coordinate directions of the aforementioned tangential fan can be further divided into a positive direction (upper light) and a negative direction (lower light). The longest operation wavelength which passes through the edge of the aperture has an imaging position on the image plane in a particular field of view, and the reference wavelength of the mail light (e.g., 555 nm) has another imaging position on the image plane in the same field of view. The transverse aberration caused when the longest operation wavelength passes through the edge of the aperture is defined as a distance between these two imaging positions. Similarly, the shortest operation wavelength which passes through the edge of the aperture has an imaging position on the image plane in a particular field of view, and the transverse aberration caused when the shortest operation wavelength passes through the edge of the aperture is defined as a distance between the imaging position of the shortest operation wavelength and the imaging position of the reference wavelength. The performance of the optical image capturing system can be considered excellent if the transverse aberrations of the shortest and the longest operation wavelength which pass through the edge of the aperture and image on the image plane in 0.7 field of view (i.e., 0.7 times the height for image formation HOI) are both less than 100 μm. Furthermore, for a stricter evaluation, the performance cannot be considered excellent unless the transverse aberrations of the shortest and the longest operation wavelength which pass through the edge of the aperture and image on the image plane in 0.7 field of view are both less than 80 μm.

The optical image capturing system has a maximum image height HOI on the image plane vertical to the optical axis. A transverse aberration at 0.7 HOI in the positive direction of the tangential fan after the longest operation wavelength of visible light passing through the edge of the aperture is denoted by PLTA; a transverse aberration at 0.7 HOI in the positive direction of the tangential fan after the shortest operation wavelength of visible light passing through the edge of the aperture is denoted by PSTA; a transverse aberration at 0.7 HOI in the negative direction of the tangential fan after the longest operation wavelength of visible light passing through the edge of the aperture is denoted by NLTA; a transverse aberration at 0.7 HOI in the negative direction of the tangential fan after the shortest operation wavelength of visible light passing through the edge of the aperture is denoted by NSTA; a transverse aberration at 0.7 HOI of the sagittal fan after the longest operation wavelength of visible light passing through the edge of the aperture is denoted by SLTA; a transverse aberration at 0.7 HOI of the sagittal fan after the shortest operation wavelength of visible light passing through the edge of the aperture is denoted by SSTA.

The present invention provides an optical image capturing system capable of focusing for both visible light and infrared light (i.e., dual mode) with certain performance, in which the seveth lens is provided with an inflection point at the object-side surface or at the image-side surface to adjust the incident angle of each view field and modify the ODT and the TDT. In addition, the surfaces of the seventh lens are capable of modifying the optical path to improve the imagining quality.

The optical image capturing system of the present invention includes a first lens, a second lens, a third lens, a fourth lens, a fifth lens, a sixth lens, a seventh lens, and an image plane in order along an optical axis from an object side to an image side. The first lens has refractive power. The optical image capturing system satisfies:

1.2≦f/HEP≦10.0; 0<InTL/HOS<0.9; and 0.9≦2(ARE/HEP)≦1.5;

where f1, f2, f3, f4, f5, f6, and f7 are respectively the focal lengths of the first lens to the seventh lens; f is a focal length of the optical image capturing system; HEP is an entrance pupil diameter of the optical image capturing system; HOS is a distance in parallel with the optical axis between an object-side surface, which face the object side, of the first lens and the image plane; InTL is a distance between the object-side surface of the first lens and the image-side surface of the seventh lens on the optical axis; ARE is a profile curve length measured from a start point where the optical axis of the belonging optical image capturing system passes through the surface of the lens, along a surface profile of the lens, and finally to a coordinate point of a perpendicular distance where is a half of the entrance pupil diameter away from the optical axis.

The present invention further provides an optical image capturing system, including a first lens, a second lens, a third lens, a fourth lens, a fifth lens, a sixth lens, a seventh lens, and an image plane in order along an optical axis from an object side to an image side. The first lens has positive refractive power, wherein the object-side surface thereof can be convex near the optical axis. The second lens has refractive power. The third lens has refractive power. The fourth lens has refractive power. The fifth lens has refractive power. The sixth lens has refractive power. The seventh lens has refractive power, wherein the object-side surface and the image-side surface thereof are both aspheric surfaces. Each of at least two lenses among the first lens to the seventh lens has at least an inflection point on at least a surface thereof. At least one lens between the second lens and the seventh lens has positive refractive power. The optical image capturing system satisfies:

1.2≦f/HEP≦10.0; 0<InTL/HOS<0.9; and 0.9≦2(ARE/HEP)≦1.5;

where f1, f2, f3, f4, f5, f6, and f7 are respectively the focal lengths of the first lens to the seventh lens; f is a focal length of the optical image capturing system; HEP is an entrance pupil diameter of the optical image capturing system; HOS is a distance in parallel with the optical axis between an object-side surface, which face the object side, of the first lens and the image plane; InTL is a distance between the object-side surface of the first lens and the image-side surface of the seventh lens on the optical axis; ARE is a profile curve length measured from a start point where the optical axis of the belonging optical image capturing system passes through the surface of the lens, along a surface profile of the lens, and finally to a coordinate point of a perpendicular distance where is a half of the entrance pupil diameter away from the optical axis.

The present invention further provides an optical image capturing system, including a first lens, a second lens, a third lens, a fourth lens, a fifth lens, a sixth lens, a seventh lens, and an image plane, in order along an optical axis from an object side to an image side. The number of the lenses having refractive power in the optical image capturing system is seven. Each of at least two lenses among the first to the seventh lenses has at least an inflection point. At least a surface of at least a lens among the first lens to the seventh lens has at least two inflection points. The first lens has positive refractive power, and the second lens has negative refractive power. The third lens has refractive power. The fourth lens has refractive power. The fifth lens has refractive power. The sixth lens has refractive power. The seventh lens has refractive power. The optical image capturing system satisfies:

1.2≦f/HEP≦3.5; 0<InTL/HOS<0.9; and 0.9≦2(ARE/HEP)≦1.5;

where f1, f2, f3, f4, f5, f6, and f7 are respectively the focal lengths of the first lens to the seventh lens; f is a focal length of the optical image capturing system; HEP is an entrance pupil diameter of the optical image capturing system; HOS is a distance in parallel with the optical axis between an object-side surface, which face the object side, of the first lens and the image plane; InTL is a distance between the object-side surface of the first lens and the image-side surface of the seventh lens on the optical axis; ARE is a profile curve length measured from a start point where the optical axis of the belonging optical image capturing system passes through the surface of the lens, along a surface profile of the lens, and finally to a coordinate point of a perpendicular distance where is a half of the entrance pupil diameter away from the optical axis.

For any surface of any lens, the profile curve length within the effective half diameter affects the ability of the surface to correct aberration and differences between optical paths of light in different fields of view. With longer profile curve length, the ability to correct aberration is better. However, the difficulty of manufacturing increases as well. Therefore, the profile curve length within the effective half diameter of any surface of any lens has to be controlled. The ratio between the profile curve length (ARS) within the effective half diameter of one surface and the thickness (TP) of the lens, which the surface belonged to, on the optical axis (i.e., ARS/TP) has to be particularly controlled. For example, the profile curve length of the maximum effective half diameter of the object-side surface of the first lens is denoted by ARS11, the thickness of the first lens on the optical axis is TP1, and the ratio between these two parameters is ARS11/TP1; the profile curve length of the maximum effective half diameter of the image-side surface of the first lens is denoted by ARS12, and the ratio between ARS12 and TP1 is ARS12/TP1. The profile curve length of the maximum effective half diameter of the object-side surface of the second lens is denoted by ARS21, the thickness of the second lens on the optical axis is TP2, and the ratio between these two parameters is ARS21/TP2; the profile curve length of the maximum effective half diameter of the image-side surface of the second lens is denoted by ARS22, and the ratio between ARS22 and TP2 is ARS22/TP2. For any surface of other lenses in the optical image capturing system, the ratio between the profile curve length of the maximum effective half diameter thereof and the thickness of the lens which the surface belonged to is denoted in the same manner.

For any surface of any lens, the profile curve length within a half of the entrance pupil diameter (HEP) affects the ability of the surface to correct aberration and differences between optical paths of light in different fields of view. With longer profile curve length, the ability to correct aberration is better. However, the difficulty of manufacturing increases as well. Therefore, the profile curve length within a half of the entrance pupil diameter (HEP) of any surface of any lens has to be controlled. The ratio between the profile curve length (ARE) within a half of the entrance pupil diameter (HEP) of one surface and the thickness (TP) of the lens, which the surface belonged to, on the optical axis (i.e., ARE/TP) has to be particularly controlled. For example, the profile curve length of a half of the entrance pupil diameter (HEP) of the object-side surface of the first lens is denoted by ARE11, the thickness of the first lens on the optical axis is TP1, and the ratio between these two parameters is ARE11/TP1; the profile curve length of a half of the entrance pupil diameter (HEP) of the image-side surface of the first lens is denoted by ARE12, and the ratio between ARE12 and TP1 is ARE12/TP1. The profile curve length of a half of the entrance pupil diameter (HEP) of the object-side surface of the second lens is denoted by ARE21, the thickness of the second lens on the optical axis is TP2, and the ratio between these two parameters is ARE21/TP2; the profile curve length of a half of the entrance pupil diameter (HEP) of the image-side surface of the second lens is denoted by ARE22, and the ratio between ARE22 and TP2 is ARE22/TP2. For any surface of other lenses in the optical image capturing system, the ratio between the profile curve length of a half of the entrance pupil diameter (HEP) thereof and the thickness of the lens which the surface belonged to is denoted in the same manner.

In an embodiment, a height of the optical image capturing system (HOS) can be reduced if |f1|>|f7|.

In an embodiment, when |f2|+|f3|+|f4|+|f5|+|f6| and |f1|+|f7| of the lenses satisfy the aforementioned conditions, at least one lens among the second to the sixth lenses could have weak positive refractive power or weak negative refractive power. Herein the weak refractive power means the absolute value of the focal length of one specific lens is greater than 10. When at least one lens among the second to the sixth lenses has weak positive refractive power, it may share the positive refractive power of the first lens, and on the contrary, when at least one lens among the second to the sixth lenses has weak negative refractive power, it may fine turn and correct the aberration of the system.

In an embodiment, the seventh lens could have negative refractive power, and an image-side surface thereof is concave, it may reduce back focal length and size. Besides, the seventh lens can have at least an inflection point on at least a surface thereof, which may reduce an incident angle of the light of an off-axis field of view and correct the aberration of the off-axis field of view.

BRIEF DESCRIPTION OF THE SEVERAL VIEWS OF THE DRAWINGS

The present invention will be best understood by referring to the following detailed description of some illustrative embodiments in conjunction with the accompanying drawings, in which

FIG. 1A is a schematic diagram of a first embodiment of the present invention;

FIG. 1B shows curve diagrams of longitudinal spherical aberration, astigmatic field, and optical distortion of the optical image capturing system in the order from left to right of the first embodiment of the present application;

FIG. 1C shows a tangential fan and a sagittal fan of the optical image capturing system of the first embodiment of the present application, and a transverse aberration diagram at 0.7 field of view when a longest operation wavelength and a shortest operation wavelength pass through an edge of an aperture;

FIG. 2A is a schematic diagram of a second embodiment of the present invention;

FIG. 2B shows curve diagrams of longitudinal spherical aberration, astigmatic field, and optical distortion of the optical image capturing system in the order from left to right of the second embodiment of the present application;

FIG. 2C shows a tangential fan and a sagittal fan of the optical image capturing system of the second embodiment of the present application, and a transverse aberration diagram at 0.7 field of view when a longest operation wavelength and a shortest operation wavelength pass through an edge of an aperture;

FIG. 3A is a schematic diagram of a third embodiment of the present invention;

FIG. 3B shows curve diagrams of longitudinal spherical aberration, astigmatic field, and optical distortion of the optical image capturing system in the order from left to right of the third embodiment of the present application;

FIG. 3C shows a tangential fan and a sagittal fan of the optical image capturing system of the third embodiment of the present application, and a transverse aberration diagram at 0.7 field of view when a longest operation wavelength and a shortest operation wavelength pass through an edge of an aperture;

FIG. 4A is a schematic diagram of a fourth embodiment of the present invention;

FIG. 4B shows curve diagrams of longitudinal spherical aberration, astigmatic field, and optical distortion of the optical image capturing system in the order from left to right of the fourth embodiment of the present application;

FIG. 4C shows a tangential fan and a sagittal fan of the optical image capturing system of the fourth embodiment of the present application, and a transverse aberration diagram at 0.7 field of view when a longest operation wavelength and a shortest operation wavelength pass through an edge of an aperture;

FIG. 5A is a schematic diagram of a fifth embodiment of the present invention;

FIG. 5B shows curve diagrams of longitudinal spherical aberration, astigmatic field, and optical distortion of the optical image capturing system in the order from left to right of the fifth embodiment of the present application;

FIG. 5C shows a tangential fan and a sagittal fan of the optical image capturing system of the fifth embodiment of the present application, and a transverse aberration diagram at 0.7 field of view when a longest operation wavelength and a shortest operation wavelength pass through an edge of an aperture;

FIG. 6A is a schematic diagram of a sixth embodiment of the present invention;

FIG. 6B shows curve diagrams of longitudinal spherical aberration, astigmatic field, and optical distortion of the optical image capturing system in the order from left to right of the sixth embodiment of the present application;

FIG. 6C shows a tangential fan and a sagittal fan of the optical image capturing system of the sixth embodiment of the present application, and a transverse aberration diagram at 0.7 field of view when a longest operation wavelength and a shortest operation wavelength pass through an edge of an aperture;

FIG. 7A is a schematic diagram of a seventh embodiment of the present invention;

FIG. 7B shows curve diagrams of longitudinal spherical aberration, astigmatic field, and optical distortion of the optical image capturing system in the order from left to right of the seventh embodiment of the present application;

FIG. 7C shows a tangential fan and a sagittal fan of the optical image capturing system of the seventh embodiment of the present application, and a transverse aberration diagram at 0.7 field of view when a longest operation wavelength and a shortest operation wavelength pass through an edge of an aperture;

FIG. 8A is a schematic diagram of a eighth embodiment of the present invention;

FIG. 8B shows curve diagrams of longitudinal spherical aberration, astigmatic field, and optical distortion of the optical image capturing system in the order from left to right of the eighth embodiment of the present application; and

FIG. 8C shows a tangential fan and a sagittal fan of the optical image capturing system of the eighth embodiment of the present application, and a transverse aberration diagram at 0.7 field of view when a longest operation wavelength and a shortest operation wavelength pass through an edge of an aperture.

DETAILED DESCRIPTION OF THE INVENTION

An optical image capturing system of the present invention includes a first lens, a second lens, a third lens, a fourth lens, a fifth lens, a sixth lens, a seventh lens, and an image plane from an object side to an image side. The optical image capturing system further is provided with an image sensor at an image plane, wherein the image heights of the following embodiments are all around 3.91 mm.

The optical image capturing system can work in three wavelengths, including 486.1 nm, 587.5 nm, and 656.2 nm, wherein 587.5 nm is the main reference wavelength and is the reference wavelength for obtaining the technical characters. The optical image capturing system can also work in five wavelengths, including 470 nm, 510 nm, 555 nm, 610 nm, and 650 nm wherein 555 nm is the main reference wavelength, and is the reference wavelength for obtaining the technical characters.

The optical image capturing system of the present invention satisfies 0.5≦τPPR/|ΣNPR|≦15, and a preferable range is 1≦ΣPPR/|ΣNPR|≦3.0, where PPR is a ratio of the focal length f of the optical image capturing system to a focal length fp of each of lenses with positive refractive power; NPR is a ratio of the focal length f of the optical image capturing system to a focal length fn of each of lenses with negative refractive power; ΣPPR is a sum of the PPRs of each positive lens; and ΣNPR is a sum of the NPRs of each negative lens. It is helpful for control of an entire refractive power and an entire length of the optical image capturing system.

The image sensor is provided on the image plane. The optical image capturing system of the present invention satisfies HOS/HOI≦10; and 0.5≦HOS/f≦10, and a preferable range is 1≦HOS/HOI≦5; and 1≦HOS/f≦7, where HOI is a half of a diagonal of an effective sensing area of the image sensor, i.e., the maximum image height, and HOS is a height of the optical image capturing system, i.e. a distance on the optical axis between the object-side surface of the first lens and the image plane. It is helpful for reduction of the size of the system for used in compact cameras.

The optical image capturing system of the present invention further is provided with an aperture to increase image quality.

In the optical image capturing system of the present invention, the aperture could be a front aperture or a middle aperture, wherein the front aperture is provided between the object and the first lens, and the middle is provided between the first lens and the image plane. The front aperture provides a long distance between an exit pupil of the system and the image plane, which allows more elements to be installed. The middle could enlarge a view angle of view of the system and increase the efficiency of the image sensor. The optical image capturing system satisfies 0.2≦InS/HOS≦1.1, where InS is a distance between the aperture and the image-side surface of the sixth lens. It is helpful for size reduction and wide angle.

The optical image capturing system of the present invention satisfies 0.1<ΣTP/InTL≦0.9, where InTL is a distance between the object-side surface of the first lens and the image-side surface of the seventh lens, and ΣTP is a sum of central thicknesses of the lenses on the optical axis. It is helpful for the contrast of image and yield rate of manufacture and provides a suitable back focal length for installation of other elements.

The optical image capturing system of the present invention satisfies 0.001≦|R1/R2|≦20, and a preferable range is 0.01≦|R1/R2|<10, where R1 is a radius of curvature of the object-side surface of the first lens, and R2 is a radius of curvature of the image-side surface of the first lens. It provides the first lens with a suitable positive refractive power to reduce the increase rate of the spherical aberration.

The optical image capturing system of the present invention satisfies −7<(R13−R14)/(R13+R14)<50, where R13 is a radius of curvature of the object-side surface of the seventh lens, and R14 is a radius of curvature of the image-side surface of the seventh lens. It may modify the astigmatic field curvature.

The optical image capturing system of the present invention satisfies IN12/f≦3.0, where IN12 is a distance on the optical axis between the first lens and the second lens. It may correct chromatic aberration and improve the performance.

The optical image capturing system of the present invention satisfies IN67/f≦0.8, where IN67 is a distance on the optical axis between the sixth lens and the seventh lens. It may correct chromatic aberration and improve the performance.

The optical image capturing system of the present invention satisfies 0.1≦(TP1+IN12)/TP2≦10, where TP1 is a central thickness of the first lens on the optical axis, and TP2 is a central thickness of the second lens on the optical axis. It may control the sensitivity of manufacture of the system and improve the performance.

The optical image capturing system of the present invention satisfies 0.1≦(TP7+IN67)/TP6≦10, where TP6 is a central thickness of the sixth lens on the optical axis, TP7 is a central thickness of the seventh lens on the optical axis, and IN67 is a distance between the sixth lens and the seventh lens. It may control the sensitivity of manufacture of the system and improve the performance.

The optical image capturing system of the present invention satisfies 0.1≦TP4/(IN34+TP4+IN45)<1, where TP3 is a central thickness of the third lens on the optical axis, TP4 is a central thickness of the fourth lens on the optical axis, TP5 is a central thickness of the fifth lens on the optical axis, IN34 is a distance on the optical axis between the third lens and the fourth lens, IN45 is a distance on the optical axis between the fourth lens and the fifth lens, and InTL is a distance between the object-side surface of the first lens and the image-side surface of the seventh lens. It may fine tune and correct the aberration of the incident rays layer by layer, and reduce the height of the system.

The optical image capturing system satisfies 0 mm≦HVT71≦3 mm; 0 mm<HVT72≦6 mm; 0≦HVT71/HVT72; 0 mm<|SGC71|≦0.5 mm; 0 mm<|SGC72|≦2 mm; and 0<|SGC72|/(|SGC72|+TP7)≦0.9, where HVT71 a distance perpendicular to the optical axis between the critical point C71 on the object-side surface of the seventh lens and the optical axis; HVT72 a distance perpendicular to the optical axis between the critical point C72 on the image-side surface of the seventh lens and the optical axis; SGC71 is a distance in parallel with the optical axis between an point on the object-side surface of the seventh lens where the optical axis passes through and the critical point C71; SGC72 is a distance in parallel with the optical axis between an point on the image-side surface of the seventh lens where the optical axis passes through and the critical point C72. It is helpful to correct the off-axis view field aberration.

The optical image capturing system satisfies 0.2≦HVT72/HOI≦0.9, and preferably satisfies 0.3≦HVT72/HOI≦0.8. It may help to correct the peripheral aberration.

The optical image capturing system satisfies 0≦HVT72/HOS≦0.5, and preferably satisfies 0.2≦HVT72/HOS≦0.45. It may help to correct the peripheral aberration.

The optical image capturing system of the present invention satisfies 0<SGI711/(SGI711+TP7)≦0.9; 0<SGI721/(SGI721+TP7)≦0.9, and it is preferable to satisfy 0.1≦SGI711/(SGI711+TP7)≦0.6; 0.1<SGI721/(SGI721+TP7)≦0.6, where SGI711 is a displacement in parallel with the optical axis, from a point on the object-side surface of the seventh lens, through which the optical axis passes, to the inflection point on the object-side surface, which is the closest to the optical axis, and SGI721 is a displacement in parallel with the optical axis, from a point on the image-side surface of the seventh lens, through which the optical axis passes, to the inflection point on the image-side surface, which is the closest to the optical axis.

The optical image capturing system of the present invention satisfies 0<SGI712/(SGI712+TP7)≦0.9; 0<SGI722/(SGI722+TP7)≦0.9, and it is preferable to satisfy 0.1≦SGI712/(SGI712+TP7)≦0.6; 0.1≦SGI722/(SGI722+TP7)≦0.6, where SGI712 is a displacement in parallel with the optical axis, from a point on the object-side surface of the seventh lens, through which the optical axis passes, to the inflection point on the object-side surface, which is the second closest to the optical axis, and SGI722 is a displacement in parallel with the optical axis, from a point on the image-side surface of the seventh lens, through which the optical axis passes, to the inflection point on the image-side surface, which is the second closest to the optical axis.

The optical image capturing system of the present invention satisfies 0.001 mm≦|HIF711|≦5 mm; 0.001 mm≦|HIF721|≦5 mm, and it is preferable to satisfy 0.1 mm≦|HIF711|≦3.5 mm; 1.5 mm≦|HIF721|≦3.5 mm, where HIF711 is a distance perpendicular to the optical axis between the inflection point on the object-side surface of the seventh lens, which is the closest to the optical axis, and the optical axis; HIF721 is a distance perpendicular to the optical axis between the inflection point on the image-side surface of the seventh lens, which is the closest to the optical axis, and the optical axis.

The optical image capturing system of the present invention satisfies 0.001 mm≦|HIF712|≦5 mm; 0.001 mm≦|HIF722|≦5 mm, and it is preferable to satisfy 0.1 mm≦|HIF722|≦3.5 mm; 0.1 mm≦|HIF712|≦3.5 mm, where HIF712 is a distance perpendicular to the optical axis between the inflection point on the object-side surface of the seventh lens, which is the second closest to the optical axis, and the optical axis; HIF722 is a distance perpendicular to the optical axis between the inflection point on the image-side surface of the seventh lens, which is the second closest to the optical axis, and the optical axis.

The optical image capturing system of the present invention satisfies 0.001 mm≦|HIF713|≦5 mm; 0.001 mm≦|HIF723|≦5 mm, and it is preferable to satisfy 0.1 mm≦|HIF723|≦3.5 mm; 0.1 mm≦|HIF713|≦3.5 mm, where HIF713 is a distance perpendicular to the optical axis between the inflection point on the object-side surface of the seventh lens, which is the third closest to the optical axis, and the optical axis; HIF723 is a distance perpendicular to the optical axis between the inflection point on the image-side surface of the seventh lens, which is the third closest to the optical axis, and the optical axis.

The optical image capturing system of the present invention satisfies 0.001 mm≦|HIF714|≦5 mm; 0.001 mm≦|HIF724|≦5 mm, and it is preferable to satisfy 0.1 mm≦|HIF724|≦3.5 mm; 0.1 mm≦|HIF714|≦3.5 mm, where HIF714 is a distance perpendicular to the optical axis between the inflection point on the object-side surface of the seventh lens, which is the fourth closest to the optical axis, and the optical axis; HIF724 is a distance perpendicular to the optical axis between the inflection point on the image-side surface of the seventh lens, which is the fourth closest to the optical axis, and the optical axis.

In an embodiment, the lenses of high Abbe number and the lenses of low Abbe number are arranged in an interlaced arrangement that could be helpful for correction of aberration of the system.

An equation of aspheric surface is

z=ch ²/[1+[1(k+1)c ² h ²]^(0.5) ]+A4h ⁴ +A6h ⁶ +A8h ⁸ +A10h ¹⁰ +A12h ¹² +A14h ¹⁴ +A16h ¹⁶ +A18h ¹⁸ +A20h ²⁰+ . . .   (1)

where z is a depression of the aspheric surface; k is conic constant; c is reciprocal of the radius of curvature; and A4, A6, A8, A10, A12, A14, A16, A18, and A20 are high-order aspheric coefficients.

In the optical image capturing system, the lenses could be made of plastic or glass. The plastic lenses may reduce the weight and lower the cost of the system, and the glass lenses may control the thermal effect and enlarge the space for arrangement of the refractive power of the system. In addition, the opposite surfaces (object-side surface and image-side surface) of the first to the seventh lenses could be aspheric that can obtain more control parameters to reduce aberration. The number of aspheric glass lenses could be less than the conventional spherical glass lenses, which is helpful for reduction of the height of the system.

When the lens has a convex surface, which means that the surface is convex around a position, through which the optical axis passes, and when the lens has a concave surface, which means that the surface is concave around a position, through which the optical axis passes.

The optical image capturing system of the present invention could be applied in a dynamic focusing optical system. It is superior in the correction of aberration and high imaging quality so that it could be allied in lots of fields.

The optical image capturing system of the present invention could further include a driving module to meet different demands, wherein the driving module can be coupled with the lenses to move the lenses. The driving module can be a voice coil motor (VCM), which is used to move the lens for focusing, or can be an optical image stabilization (OIS) component, which is used to lower the possibility of having the problem of image blurring which is caused by subtle movements of the lens while shooting.

To meet different requirements, at least one lens among the first lens to the seventh lens of the optical image capturing system of the present invention can be a light filter, which filters out light of wavelength shorter than 500 nm. Such effect can be achieved by coating on at least one surface of the lens, or by using materials capable of filtering out short waves to make the lens.

We provide several embodiments in conjunction with the accompanying drawings for the best understanding, which are:

First Embodiment

As shown in FIG. 1A and FIG. 1B, an optical image capturing system 10 of the first embodiment of the present invention includes, along an optical axis from an object side to an image side, a first lens 110, an aperture 100, a second lens 120, a third lens 130, a fourth lens 140, a fifth lens 150, a sixth lens 160, a seventh lens 170, an infrared rays filter 180, an image plane 190, and an image sensor 192. FIG. 1C shows a tangential fan and a sagittal fan of the optical image capturing system 10 of the first embodiment of the present application, and a transverse aberration diagram at 0.7 field of view when a longest operation wavelength and a shortest operation wavelength pass through an edge of the aperture 100.

The first lens 110 has negative refractive power and is made of plastic. An object-side surface 112 thereof, which faces the object side, is a concave aspheric surface, and an image-side surface 114 thereof, which faces the image side, is a concave aspheric surface. The object-side surface 112 has an inflection point, and the image-side surface 114 has two inflection points. A profile curve length of the maximum effective half diameter of an object-side surface of the first lens 110 is denoted by ARS11, and a profile curve length of the maximum effective half diameter of the image-side surface of the first lens 110 is denoted by ARS12. A profile curve length of a half of an entrance pupil diameter (HEP) of the object-side surface of the first lens 110 is denoted by ARE11, and a profile curve length of a half of the entrance pupil diameter (HEP) of the image-side surface of the first lens 110 is denoted by ARE12. A thickness of the first lens 110 on the optical axis is TP1.

The first lens 110 satisfies SGI111=−0.1110 mm; SGI121=2.7120 mm; TP1=2.2761 mm; |SGI111|/(|SGI111|+TP1)=0.0465; |SGI121|/(|SGI121|+TP1)=0.5437, where a displacement in parallel with the optical axis from a point on the object-side surface of the first lens, through which the optical axis passes, to the inflection point on the image-side surface, which is the closest to the optical axis is denoted by SGI111, and a displacement in parallel with the optical axis from a point on the image-side surface of the first lens, through which the optical axis passes, to the inflection point on the image-side surface, which is the closest to the optical axis is denoted by SGI121.

The first lens 110 satisfies SGI112=0 mm; SGI122=4.2315 mm; |SGI112|/(|SGI112|+TP1)=0; |SGI122|/(|SGI122|+TP1)=0.6502, where a displacement in parallel with the optical axis from a point on the object-side surface of the first lens, through which the optical axis passes, to the inflection point on the image-side surface, which is the second closest to the optical axis is denoted by SGI112, and a displacement in parallel with the optical axis from a point on the image-side surface of the first lens, through which the optical axis passes, to the inflection point on the image-side surface, which is the second closest to the optical axis is denoted by SGI122.

The first lens 110 satisfies HIF111=12.8432 mm; HIF111/HOI=1.7127; HIF121=7.1744 mm; HIF121/HOI=0.9567, where a displacement perpendicular to the optical axis from a point on the object-side surface of the first lens, through which the optical axis passes, to the inflection point, which is the closest to the optical axis is denoted by HIF111, and a displacement perpendicular to the optical axis from a point on the image-side surface of the first lens, through which the optical axis passes, to the inflection point, which is the closest to the optical axis is denoted by HIF121.

The first lens 110 satisfies HIF112=0 mm; HIF112/HOI=0; HIF122=9.8592 mm; HIF122/HOI=1.3147, where a displacement perpendicular to the optical axis from a point on the object-side surface of the first lens, through which the optical axis passes, to the inflection point, which is the second closest to the optical axis is denoted by HIF112, and a displacement perpendicular to the optical axis from a point on the image-side surface of the first lens, through which the optical axis passes, to the inflection point, which is the second closest to the optical axis is denoted by HIF122.

The second lens 120 has positive refractive power and is made of plastic. An object-side surface 122 thereof, which faces the object side, is a convex aspheric surface, and an image-side surface 124 thereof, which faces the image side, is a concave aspheric surface. A profile curve length of the maximum effective half diameter of an object-side surface of the second lens 120 is denoted by ARS21, and a profile curve length of the maximum effective half diameter of the image-side surface of the second lens 120 is denoted by ARS22. A profile curve length of a half of an entrance pupil diameter (HEP) of the object-side surface of the second lens 120 is denoted by ARE21, and a profile curve length of a half of the entrance pupil diameter (HEP) of the image-side surface of the second lens 120 is denoted by ARE22. A thickness of the second lens 120 on the optical axis is TP2.

For the second lens 120, a displacement in parallel with the optical axis from a point on the object-side surface of the second lens, through which the optical axis passes, to the inflection point on the image-side surface, which is the closest to the optical axis is denoted by SGI211, and a displacement in parallel with the optical axis from a point on the image-side surface of the second lens, through which the optical axis passes, to the inflection point on the image-side surface, which is the closest to the optical axis is denoted by SGI221.

For the second lens, a displacement perpendicular to the optical axis from a point on the object-side surface of the second lens, through which the optical axis passes, to the inflection point, which is the closest to the optical axis is denoted by HIF211, and a displacement perpendicular to the optical axis from a point on the image-side surface of the second lens, through which the optical axis passes, to the inflection point, which is the closest to the optical axis is denoted by HIF221.

The third lens 130 has negative refractive power and is made of plastic. An object-side surface 132, which faces the object side, is a convex aspheric surface, and an image-side surface 134, which faces the image side, is a concave aspheric surface. A profile curve length of the maximum effective half diameter of an object-side surface of the third lens 130 is denoted by ARS31, and a profile curve length of the maximum effective half diameter of the image-side surface of the third lens 130 is denoted by ARS32. A profile curve length of a half of an entrance pupil diameter (HEP) of the object-side surface of the third lens 130 is denoted by ARE31, and a profile curve length of a half of the entrance pupil diameter (HEP) of the image-side surface of the third lens 130 is denoted by ARE32. A thickness of the third lens 130 on the optical axis is TP3.

For the third lens 130, SGI311 is a displacement in parallel with the optical axis, from a point on the object-side surface of the third lens, through which the optical axis passes, to the inflection point on the object-side surface, which is the closest to the optical axis, and SGI321 is a displacement in parallel with the optical axis, from a point on the image-side surface of the third lens, through which the optical axis passes, to the inflection point on the image-side surface, which is the closest to the optical axis.

For the third lens 130, SGI312 is a displacement in parallel with the optical axis, from a point on the object-side surface of the third lens, through which the optical axis passes, to the inflection point on the object-side surface, which is the second closest to the optical axis, and SGI322 is a displacement in parallel with the optical axis, from a point on the image-side surface of the third lens, through which the optical axis passes, to the inflection point on the object-side surface, which is the second closest to the optical axis.

For the third lens 130, HIF311 is a distance perpendicular to the optical axis between the inflection point on the object-side surface of the third lens, which is the closest to the optical axis, and the optical axis; HIF321 is a distance perpendicular to the optical axis between the inflection point on the image-side surface of the third lens, which is the closest to the optical axis, and the optical axis.

For the third lens 130, HIF312 is a distance perpendicular to the optical axis between the inflection point on the object-side surface of the third lens, which is the second closest to the optical axis, and the optical axis; HIF322 is a distance perpendicular to the optical axis between the inflection point on the image-side surface of the third lens, which is the second closest to the optical axis, and the optical axis.

The fourth lens 140 has positive refractive power and is made of plastic. An object-side surface 142, which faces the object side, is a convex aspheric surface, and an image-side surface 144, which faces the image side, is a convex aspheric surface. The object-side surface 142 has an inflection point. A profile curve length of the maximum effective half diameter of an object-side surface of the fourth lens 140 is denoted by ARS41, and a profile curve length of the maximum effective half diameter of the image-side surface of the fourth lens 140 is denoted by ARS42. A profile curve length of a half of an entrance pupil diameter (HEP) of the object-side surface of the fourth lens 140 is denoted by ARE41, and a profile curve length of a half of the entrance pupil diameter (HEP) of the image-side surface of the fourth lens 140 is denoted by ARE42. A thickness of the fourth lens 140 on the optical axis is TP4.

The fourth lens 140 satisfies SGI411=0.0018 mm; |SGI411|/(|SGI411|+TP4)=0.0009, where SGI411 is a displacement in parallel with the optical axis, from a point on the object-side surface of the fourth lens, through which the optical axis passes, to the inflection point on the object-side surface, which is the closest to the optical axis, and SGI421 is a displacement in parallel with the optical axis, from a point on the image-side surface of the fourth lens, through which the optical axis passes, to the inflection point on the image-side surface, which is the closest to the optical axis.

For the fourth lens 140, SGI412 is a displacement in parallel with the optical axis, from a point on the object-side surface of the fourth lens, through which the optical axis passes, to the inflection point on the object-side surface, which is the second closest to the optical axis, and SGI422 is a displacement in parallel with the optical axis, from a point on the image-side surface of the fourth lens, through which the optical axis passes, to the inflection point on the object-side surface, which is the second closest to the optical axis.

The fourth lens 140 further satisfies HIF411=0.7191 mm; HIF411/HOI=0.0959, where HIF411 is a distance perpendicular to the optical axis between the inflection point on the object-side surface of the fourth lens, which is the closest to the optical axis, and the optical axis; HIF421 is a distance perpendicular to the optical axis between the inflection point on the image-side surface of the fourth lens, which is the closest to the optical axis, and the optical axis.

For the fourth lens 140, HIF412 is a distance perpendicular to the optical axis between the inflection point on the object-side surface of the fourth lens, which is the second closest to the optical axis, and the optical axis; HIF422 is a distance perpendicular to the optical axis between the inflection point on the image-side surface of the fourth lens, which is the second closest to the optical axis, and the optical axis.

The fifth lens 150 has positive refractive power and is made of plastic. An object-side surface 152, which faces the object side, is a concave aspheric surface, and an image-side surface 154, which faces the image side, is a convex aspheric surface. The object-side surface 152 and the image-side surface 154 both have an inflection point. A profile curve length of the maximum effective half diameter of an object-side surface of the fifth lens 150 is denoted by ARS51, and a profile curve length of the maximum effective half diameter of the image-side surface of the fifth lens 150 is denoted by ARS52. A profile curve length of a half of an entrance pupil diameter (HEP) of the object-side surface of the fifth lens 150 is denoted by ARE51, and a profile curve length of a half of the entrance pupil diameter (HEP) of the image-side surface of the fifth lens 150 is denoted by ARE52. A thickness of the fifth lens 150 on the optical axis is TP5.

The fifth lens 150 satisfies SGI511=−0.1246 mm; SGI521=−2.1477 mm; |SGI511|/(|SGI511|+TP5)=0.0284; |SGI521|/(|SGI521|+TP5)=0.3346, where SGI511 is a displacement in parallel with the optical axis, from a point on the object-side surface of the fifth lens, through which the optical axis passes, to the inflection point on the object-side surface, which is the closest to the optical axis, and SGI521 is a displacement in parallel with the optical axis, from a point on the image-side surface of the fifth lens, through which the optical axis passes, to the inflection point on the image-side surface, which is the closest to the optical axis.

For the fifth lens 150, SGI512 is a displacement in parallel with the optical axis, from a point on the object-side surface of the fifth lens, through which the optical axis passes, to the inflection point on the object-side surface, which is the second closest to the optical axis, and SGI522 is a displacement in parallel with the optical axis, from a point on the image-side surface of the fifth lens, through which the optical axis passes, to the inflection point on the object-side surface, which is the second closest to the optical axis.

The fifth lens 150 further satisfies HIF511=3.8179 mm; HIF521=4.5480 mm; HIF511/HOI=0.5091; HIF521/HOI=0.6065, where HIF511 is a distance perpendicular to the optical axis between the inflection point on the object-side surface of the fifth lens, which is the closest to the optical axis, and the optical axis; HIF521 is a distance perpendicular to the optical axis between the inflection point on the image-side surface of the fifth lens, which is the closest to the optical axis, and the optical axis.

For the fifth lens 150, HIF512 is a distance perpendicular to the optical axis between the inflection point on the object-side surface of the fifth lens, which is the second closest to the optical axis, and the optical axis; HIF522 is a distance perpendicular to the optical axis between the inflection point on the image-side surface of the fifth lens, which is the second closest to the optical axis, and the optical axis.

The sixth lens 160 has negative refractive power and is made of plastic. An object-side surface 162, which faces the object side, is a convex surface, and an image-side surface 164, which faces the image side, is a concave surface. The object-side surface 162 and the image-side surface 164 both have an inflection point. Whereby, incident angle of each field of view for the sixth lens can be effectively adjusted to improve aberration. A profile curve length of the maximum effective half diameter of an object-side surface of the sixth lens 160 is denoted by ARS61, and a profile curve length of the maximum effective half diameter of the image-side surface of the sixth lens 160 is denoted by ARS62. A profile curve length of a half of an entrance pupil diameter (HEP) of the object-side surface of the sixth lens 160 is denoted by ARE61, and a profile curve length of a half of the entrance pupil diameter (HEP) of the image-side surface of the sixth lens 160 is denoted by ARE62. A thickness of the sixth lens 160 on the optical axis is TP6.

The sixth lens 160 satisfies SGI611=0.3208 mm; SGI621=0.5937 mm; |SGI611|/(|SGI611|+TP6)=0.5167; |SGI621|/(|SGI621|+TP6)=0.6643, where SGI611 is a displacement in parallel with the optical axis, from a point on the object-side surface of the sixth lens, through which the optical axis passes, to the inflection point on the object-side surface, which is the closest to the optical axis, and SGI621 is a displacement in parallel with the optical axis, from a point on the image-side surface of the sixth lens, through which the optical axis passes, to the inflection point on the image-side surface, which is the closest to the optical axis.

The sixth lens 160 further satisfies HIF611=1.9655 mm; HIF621=2.0041 mm; HIF611/HOI=0.2621; HIF621/HOI=0.2672, where HIF611 is a distance perpendicular to the optical axis between the inflection point on the object-side surface of the sixth lens, which is the closest to the optical axis, and the optical axis; HIF621 is a distance perpendicular to the optical axis between the inflection point on the image-side surface of the sixth lens, which is the closest to the optical axis, and the optical axis.

The seventh lens 170 has positive refractive power and is made of plastic. An object-side surface 172, which faces the object side, is a convex surface, and an image-side surface 174, which faces the image side, is a concave surface. Whereby, it is helpful to shorten the focal length behind the seventh lens for miniaturization. The object-side surface 172 and the image-side surface 174 both have an inflection point. A profile curve length of the maximum effective half diameter of an object-side surface of the seventh lens 170 is denoted by ARS71, and a profile curve length of the maximum effective half diameter of the image-side surface of the seventh lens 170 is denoted by ARS72. A profile curve length of a half of an entrance pupil diameter (HEP) of the object-side surface of the seventh lens 170 is denoted by ARE71, and a profile curve length of a half of the entrance pupil diameter (HEP) of the image-side surface of the seventh lens 170 is denoted by ARE72. A thickness of the seventh lens 170 on the optical axis is TP7.

The seventh lens 170 satisfies SGI711=0.5212 mm; SGI721=0.5668 mm; |SGI711|/(|SGI711|+TP7)=0.3179; |SGI721|/(|SGI721|+TP7)=0.3364, where SGI711 is a displacement in parallel with the optical axis, from a point on the object-side surface of the seventh lens, through which the optical axis passes, to the inflection point on the object-side surface, which is the closest to the optical axis, and SGI721 is a displacement in parallel with the optical axis, from a point on the image-side surface of the seventh lens, through which the optical axis passes, to the inflection point on the image-side surface, which is the closest to the optical axis.

The seventh lens 170 further satisfies HIF711=1.6707 mm; HIF721=1.8616 mm; HIF711/HOI=0.2228; HIF721/HOI=0.2482, where HIF711 is a distance perpendicular to the optical axis between the inflection point on the object-side surface of the seventh lens, which is the closest to the optical axis, and the optical axis; HIF721 is a distance perpendicular to the optical axis between the inflection point on the image-side surface of the seventh lens, which is the closest to the optical axis, and the optical axis.

The features related to the inflection points in the present embodiment described below are obtained with the main reference wavelength 555 nm.

The infrared rays filter 180 is made of glass and between the seventh lens 170 and the image plane 190. The infrared rays filter 180 gives no contribution to the focal length of the system.

The optical image capturing system 10 of the first embodiment has the following parameters, which are f=4.3019 mm; f/HEP=1.2; HAF=59.9968; and tan(HAF)=1.7318, where f is a focal length of the system; HAF is a half of the maximum field angle; and HEP is an entrance pupil diameter.

The parameters of the lenses of the first embodiment are f1=−14.5286 mm; |f/f1|=0.2961; f7=8.2933; |f1|>f7; and |f1/f7|=1.7519, where f1 is a focal length of the first lens 110; and f7 is a focal length of the seventh lens 170.

The first embodiment further satisfies |f2|+|f3|+|f4|+|f5|+|f6|=144.7494; |f1|+|f7|=22.8219 and |f2|+|f3|+|f4|+|f5|+|f6|>|f1|+|f7|, where f2 is a focal length of the second lens 120, f3 is a focal length of the third lens 130, f4 is a focal length of the fourth lens 140, f5 is a focal length of the fifth lens 150, f6 is a focal length of the sixth lens 160, and f7 is a focal length of the seventh lens 170.

The optical image capturing system 10 of the first embodiment further satisfies ΣPPR=f/f2+f/f4+f/f5+f/f7=1.7384; ΣNPR=f/f1+f/f3+f/f6=−0.9999; ΣPPR/|ΣNPR|=1.7386; |f/f2|=0.1774; |f/f3|=0.0443; |f/f4|=0.4411; |f/f5|=0.6012; |f/f6|=0.6595; |f/f7|=0.5187, where PPR is a ratio of a focal length f of the optical image capturing system to a focal length fp of each of the lenses with positive refractive power; and NPR is a ratio of a focal length f of the optical image capturing system to a focal length fn of each of lenses with negative refractive power.

The optical image capturing system 10 of the first embodiment further satisfies InTL+BFL=HOS; HOS=26.9789 mm; HOI=7.5 mm; HOS/HOI=3.5977; HOS/f=6.2715; InS=12.4615 mm; and InS/HOS=0.4619, where InTL is a distance between the object-side surface 112 of the first lens 110 and the image-side surface 174 of the seventh lens 170; HOS is a height of the image capturing system, i.e. a distance between the object-side surface 112 of the first lens 110 and the image plane 190; InS is a distance between the aperture 100 and the image plane 190; HOI is a half of a diagonal of an effective sensing area of the image sensor 192, i.e., the maximum image height; and BFL is a distance between the image-side surface 174 of the seventh lens 170 and the image plane 190.

The optical image capturing system 10 of the first embodiment further satisfies ΣTP=16.0446 mm; and ΣTP/InTL=0.6559, where ΣTP is a sum of the thicknesses of the lenses 110-170 with refractive power. It is helpful for the contrast of image and yield rate of manufacture and provides a suitable back focal length for installation of other elements.

The optical image capturing system 10 of the first embodiment further satisfies |R1/R2|=129.9952, where R1 is a radius of curvature of the object-side surface 112 of the first lens 110, and R2 is a radius of curvature of the image-side surface 114 of the first lens 110. It provides the first lens with a suitable positive refractive power to reduce the increase rate of the spherical aberration.

The optical image capturing system 10 of the first embodiment further satisfies (R13−R14)/(R13+R14)=−0.0806, where R13 is a radius of curvature of the object-side surface 172 of the seventh lens 170, and R14 is a radius of curvature of the image-side surface 174 of the seventh lens 170. It may modify the astigmatic field curvature.

The optical image capturing system 10 of the first embodiment further satisfies ΣPP=f2+f4+f5+f7=49.4535 mm; and f4/(f2+f4+f5+f7)=0.1972, where ΣPP is a sum of the focal lengths fp of each lens with positive refractive power. It is helpful to share the positive refractive power of the fourth lens 140 to other positive lenses to avoid the significant aberration caused by the incident rays.

The optical image capturing system 10 of the first embodiment further satisfies ΣNP=f1+f3+f6=−118.1178 mm; and f1/(f1+f3+f6)=0.1677, where ΣNP is a sum of the focal lengths fn of each lens with negative refractive power. It is helpful to share the negative refractive power of the first lens 110 to other negative lenses, which avoids the significant aberration caused by the incident rays.

The optical image capturing system 10 of the first embodiment further satisfies IN12=4.5524 mm; IN12/f=1.0582, where IN12 is a distance on the optical axis between the first lens 110 and the second lens 120. It may correct chromatic aberration and improve the performance.

The optical image capturing system 10 of the first embodiment further satisfies TP1=2.2761 mm; TP2=0.2398 mm; and (TP1+IN12)/TP2=1.3032, where TP1 is a central thickness of the first lens 110 on the optical axis, and TP2 is a central thickness of the second lens 120 on the optical axis. It may control the sensitivity of manufacture of the system and improve the performance.

The optical image capturing system 10 of the first embodiment further satisfies TP6=0.3000 mm; TP7=1.1182 mm; and (TP7+IN67)/TP6=4.4322, where TP6 is a central thickness of the sixth lens 160 on the optical axis, TP7 is a central thickness of the seventh lens 170 on the optical axis, and IN67 is a distance on the optical axis between the sixth lens 160 and the seventh lens 170. It may control the sensitivity of manufacture of the system and lower the total height of the system.

The optical image capturing system 10 of the first embodiment further satisfies TP3=0.8369 mm; TP4=2.0022 mm; TP5=4.2706 mm; IN34=1.9268 mm; IN45=1.5153 mm; and TP4/(IN34+TP4+IN45)=0.3678, where TP3 is a central thickness of the third lens 130 on the optical axis, TP4 is a central thickness of the fourth lens 140 on the optical axis, TP5 is a central thickness of the fifth lens 150 on the optical axis, IN34 is a distance on the optical axis between the third lens 130 and the fourth lens 140, and IN45 is a distance on the optical axis between the fourth lens 140 and the fifth lens 150. It may control the sensitivity of manufacture of the system and lower the total height of the system.

The optical image capturing system 10 of the first embodiment further satisfies InRS61=−0.7823 mm; InRS62=−0.2166 mm; and |InRS62|/TP6 =0.722, where InRS61 is a displacement in parallel with the optical axis from a point on the object-side surface 162 of the sixth lens 160, through which the optical axis passes, to a point at the maximum effective semi diameter of the object-side surface 162 of the sixth lens; InRS62 is a displacement in parallel with the optical axis from a point on the image-side surface 164 of the sixth lens 160, through which the optical axis passes, to a point at the maximum effective semi diameter of the image-side surface 164 of the sixth lens 160; and TP6 is a central thickness of the sixth lens 160 on the optical axis. It is helpful for manufacturing and shaping of the lenses and is helpful to reduce the size.

The optical image capturing system 10 of the first embodiment further satisfies HVT61=3.3498 mm; HVT62=3.9860 mm; and HVT61/HVT62=0.8404, where HVT61 a distance perpendicular to the optical axis between the critical point on the object-side surface 162 of the sixth lens 160 and the optical axis; and HVT62 a distance perpendicular to the optical axis between the critical point on the image-side surface 164 of the sixth lens 160 and the optical axis.

The optical image capturing system 10 of the first embodiment further satisfies InRS71=−0.2756 mm; InRS72=−0.0938 mm; and |InRS72|/TP7=0.0839, where InRS71 is a displacement in parallel with the optical axis from a point on the object-side surface 172 of the seventh lens 170, through which the optical axis passes, to a point at the maximum effective semi diameter of the object-side surface 172 of the seventh lens 170; InRS72 is a displacement in parallel with the optical axis from a point on the image-side surface 174 of the seventh lens 170, through which the optical axis passes, to a point at the maximum effective semi diameter of the image-side surface 174 of the seventh lens 170; and TP7 is a central thickness of the seventh lens 170 on the optical axis. It is helpful for manufacturing and shaping of the lenses and is helpful to reduce the size.

The optical image capturing system 10 of the first embodiment satisfies HVT71=3.6822 mm; HVT72=4.0606 mm; and HVT71/HVT72=0.9068, where HVT71 a distance perpendicular to the optical axis between the critical point on the object-side surface 172 of the seventh lens 170 and the optical axis; and HVT72 a distance perpendicular to the optical axis between the critical point on the image-side surface 174 of the seventh lens 170 and the optical axis.

The optical image capturing system 10 of the first embodiment satisfies HVT72/HOI=0.5414. It is helpful for correction of the aberration of the peripheral view field of the optical image capturing system.

The optical image capturing system 10 of the first embodiment satisfies HVT72/HOS=0.1505. It is helpful for correction of the aberration of the peripheral view field of the optical image capturing system.

The second lens 120, the third lens 130, and the seventh lens 170 have negative refractive power. The optical image capturing system 10 of the first embodiment further satisfies 1≦NA7/NA2, where NA2 is an Abbe number of the second lens 120; and NA7 is an Abbe number of the seventh lens 170. It may correct the aberration of the optical image capturing system.

The optical image capturing system 10 of the first embodiment further satisfies |TDT|=2.5678%; |ODT|=2.1302%, where TDT is TV distortion; and ODT is optical distortion.

For the fifth lens 150 of the optical image capturing system 10 in the first embodiment, a transverse aberration at 0.7 field of view in the positive direction of the tangential fan after the shortest operation wavelength of visible light passing through the edge of the aperture 100 is denoted by PSTA, and is 0.00040 mm; a transverse aberration at 0.7 field of view in the positive direction of the tangential fan after the longest operation wavelength of visible light passing through the edge of the aperture 100 is denoted by PLTA, and is −0.009 mm; a transverse aberration at 0.7 field of view in the negative direction of the tangential fan after the shortest operation wavelength of visible light passing through the edge of the aperture 100 is denoted by NSTA, and is −0.002 mm; a transverse aberration at 0.7 field of view in the negative direction of the tangential fan after the longest operation wavelength of visible light passing through the edge of the aperture 100 is denoted by NLTA, and is −0.016 mm; a transverse aberration at 0.7 field of view of the sagittal fan after the shortest operation wavelength of visible light passing through the edge of the aperture 100 is denoted by SSTA, and is 0.018 mm; a transverse aberration at 0.7 field of view of the sagittal fan after the longest operation wavelength of visible light passing through the edge of the aperture 100 is denoted by SLTA, and is 0.016 mm.

The parameters of the lenses of the first embodiment are listed in Table 1 and Table 2.

TABLE 1 f = 4.3019 mm; f/HEP = 1.2; HAF = 59.9968 deg Focal Radius of curvature Thickness Refractive Abbe length Surface (mm) (mm) Material index number (mm) 0 Object plane infinity 1 1^(st) lens −1079.499964 2.276 plastic 1.565 58.00 −14.53 2 8.304149657 4.552 3 2^(nd) lens 14.39130913 5.240 plastic 1.650 21.40 24.25 4 130.0869482 0.162 5 3^(rd) lens 8.167310118 0.837 plastic 1.650 21.40 −97.07 6 6.944477468 1.450 7 Aperture plane 0.477 8 4^(th) lens 121.5965254 2.002 plastic 1.565 58.00 9.75 9 −5.755749302 1.515 10 5^(th) lens −86.27705938 4.271 plastic 1.565 58.00 7.16 11 −3.942936258 0.050 12 6^(th) lens 4.867364751 0.300 plastic 1.650 21.40 −6.52 13 2.220604983 0.211 14 7^(th) lens 1.892510651 1.118 plastic 1.650 21.40 8.29 15 2.224128115 1.400 16 Infrared plane 0.200 BK_7 1.517 64.2 rays filter 17 plane 0.917 18 Image plane plane Reference wavelength (d-line): 555 nm.

TABLE 2 Coefficients of the aspheric surfaces Surface 1 2 3 4 5 6 8 k 2.500000E+01 −4.711931E−01 1.531617E+00 −1.153034E+01 −2.915013E+00 4.886991E+00 −3.459463E+01 A4 5.236918E−06 −2.117558E−04 7.146736E−05 4.353586E−04 5.793768E−04 −3.756697E−04 −1.292614E−03 A6 −3.014384E−08 −1.838670E−06 2.334364E−06 1.400287E−05 2.112652E−04 3.901218E−04 −1.602381E−05 A8 −2.487400E−10 9.605910E−09 −7.479362E−08 −1.688929E−07 −1.344586E−05 −4.925422E−05 −8.452359E−06 A10 1.170000E−12 −8.256000E−11 1.701570E−09 3.829807E−08 1.000482E−06 4.139741E−06 7.243999E−07 A12 0.000000E+00 0.000000E+00 0.000000E+00 0.000000E+00 0.000000E+00 0.000000E+00 0.000000E+00 A14 0.000000E+00 0.000000E+00 0.000000E+00 0.000000E+00 0.000000E+00 0.000000E+00 0.000000E+00 Surface 9 10 11 12 13 14 15 k −7.549291E+00 −5.000000E+01 −1.740728E+00 −4.709650E+00 −4.509781E+00 −3.427137E+00 −3.215123E+00 A4 −5.583548E−03 1.240671E−04 6.467538E−04 −1.872317E−03 −8.967310E−04 −3.189453E−03 −2.815022E−03 A6 1.947110E−04 −4.949077E−05 −4.981838E−05 −1.523141E−05 −2.688331E−05 −1.058126E−05 1.884580E−05 A8 −1.486947E−05 2.088854E−06 9.129031E−07 −2.169414E−06 −8.324958E−07 1.760103E−06 −1.017223E−08 A10 −6.501246E−08 −1.438383E−08 7.108550E−09 −2.308304E−08 −6.184250E−09 −4.730294E−08 3.660000E−12 A12 0.000000E+00 0.000000E+00 0.000000E+00 0.000000E+00 0.000000E+00 0.000000E+00 0.000000E+00 A14 0.000000E+00 0.000000E+00 0.000000E+00 0.000000E+00 0.000000E+00 0.000000E+00 0.000000E+00

The figures related to the profile curve lengths obtained based on Table 1 and Table 2 are listed in the following table:

First embodiment (Reference wavelength: 555 nm) ARE ½(HEP) ARE value ARE − ½(HEP) 2(ARE/HEP) % TP ARE/TP (%) 11 1.792 1.792 −0.00044 99.98% 2.276 78.73% 12 1.792 1.806 0.01319 100.74% 2.276 79.33% 21 1.792 1.797 0.00437 100.24% 5.240 34.29% 22 1.792 1.792 −0.00032 99.98% 5.240 34.20% 31 1.792 1.808 0.01525 100.85% 0.837 216.01% 32 1.792 1.819 0.02705 101.51% 0.837 217.42% 41 1.792 1.792 −0.00041 99.98% 2.002 89.50% 42 1.792 1.825 0.03287 101.83% 2.002 91.16% 51 1.792 1.792 −0.00031 99.98% 4.271 41.96% 52 1.792 1.845 0.05305 102.96% 4.271 43.21% 61 1.792 1.818 0.02587 101.44% 0.300 606.10% 62 1.792 1.874 0.08157 104.55% 0.300 624.67% 71 1.792 1.898 0.10523 105.87% 1.118 169.71% 72 1.792 1.885 0.09273 105.17% 1.118 168.59% ARS EHD ARS value ARS − EHD (ARS/EHD) % TP ARS/TP (%) 11 15.095 15.096 0.001 100.01% 2.276 663.24% 12 10.315 11.377 1.062 110.29% 2.276 499.86% 21 7.531 8.696 1.166 115.48% 5.240 165.96% 22 4.759 4.881 0.122 102.56% 5.240 93.15% 31 3.632 4.013 0.382 110.51% 0.837 479.55% 32 2.815 3.159 0.344 112.23% 0.837 377.47% 41 2.967 2.971 0.004 100.13% 2.002 148.38% 42 3.402 3.828 0.426 112.53% 2.002 191.20% 51 4.519 4.523 0.004 100.10% 4.271 105.91% 52 5.016 5.722 0.706 114.08% 4.271 133.99% 61 5.019 5.823 0.805 116.04% 0.300 1941.14% 62 5.629 6.605 0.976 117.34% 0.300 2201.71% 71 5.634 6.503 0.869 115.43% 1.118 581.54% 72 6.488 7.152 0.664 110.24% 1.118 639.59%

The detail parameters of the first embodiment are listed in Table 1, in which the unit of the radius of curvature, thickness, and focal length are millimeter, and surface 0-10 indicates the surfaces of all elements in the system in sequence from the object side to the image side. Table 2 is the list of coefficients of the aspheric surfaces, in which A1-A20 indicate the coefficients of aspheric surfaces from the first order to the twentieth order of each aspheric surface. The following embodiments have the similar diagrams and tables, which are the same as those of the first embodiment, so we do not describe it again.

Second Embodiment

As shown in FIG. 2A and FIG. 2B, an optical image capturing system 20 of the second embodiment of the present invention includes, along an optical axis from an object side to an image side, a first lens 210, a second lens 220, an aperture 200, a third lens 230, a fourth lens 240, a fifth lens 250, a sixth lens 260, a seven lens 270, an infrared rays filter 280, an image plane 290, and an image sensor 292. FIG. 2C is a transverse aberration diagram at 0.7 field of view of the second embodiment of the present application.

The first lens 210 has positive refractive power and is made of plastic. An object-side surface 212 thereof, which faces the object side, is a convex aspheric surface, and an image-side surface 214 thereof, which faces the image side, is a concave aspheric surface. The image-side surface 214 has an inflection point.

The second lens 220 has negative refractive power and is made of plastic. An object-side surface 222 thereof, which faces the object side, is a convex aspheric surface, and an image-side surface 224 thereof, which faces the image side, is a concave aspheric surface. The object-side surface 222 has an inflection point.

The third lens 230 has positive refractive power and is made of plastic. An object-side surface 232, which faces the object side, is a convex aspheric surface, and an image-side surface 234, which faces the image side, is a convex aspheric surface. The object-side surface 232 has an inflection point.

The fourth lens 240 has positive refractive power and is made of plastic. An object-side surface 242, which faces the object side, is a convex aspheric surface, and an image-side surface 244, which faces the image side, is a convex aspheric surface. The object-side surface 242 has an inflection point.

The fifth lens 250 has negative refractive power and is made of plastic. An object-side surface 252, which faces the object side, is a concave surface, and an image-side surface 254, which faces the image side, is a concave surface. The object-side surface 252 and the image-side surface 254 are both aspheric surfaces. The object-side surface 252 has an inflection point.

The sixth lens 260 has positive refractive power and is made of plastic. An object-side surface 262, which faces the object side, is a convex aspheric surface, and an image-side surface 264, which faces the image side, is a convex aspheric surface. The object-side surface 262 has an inflection point. Whereby, incident angle of each field of view for the sixth lens can be effectively adjusted to improve aberration.

The seventh lens 270 has positive refractive power and is made of plastic. An object-side surface 272, which faces the object side, is a convex surface, and an image-side surface 274, which faces the image side, is a concave surface. It may help to shorten the back focal length to keep small in size. In addition, for the seventh lens 270, the object-side surface 272 and the image-side surface 274 both have an inflection point, which may reduce an incident angle of the light of an off-axis field of view and correct the aberration of the off-axis field of view.

The infrared rays filter 280 is made of glass and between the seventh lens 270 and the image plane 290. The infrared rays filter 280 gives no contribution to the focal length of the system.

In the second embodiment, the optical image capturing system of the second embodiment further satisfies ΣPP=206.0282 mm; and f1/ΣPP=0.4715, where ΣPP is a sum of the focal lengths of each positive lens. It is helpful to share the positive refractive power of one single lens to other positive lenses to avoid the significant aberration caused by the incident rays.

The optical image capturing system of the second embodiment further satisfies ΣNP=−21.4376 mm; and f2/ΣNP=0.5052, where ΣNP is a sum of the focal lengths of each negative lens. It is helpful to share the negative refractive power of one single lens to other negative lenses.

The parameters of the lenses of the second embodiment are listed in Table 3 and Table 4.

TABLE 3 f = 7.0156 mm; f/HEP = 1.4; HAF = 47.5006 deg Focal Radius of Thickness Refractive Abbe length Surface curvature (mm) (mm) Material index number (mm) 0 Object plane infinity 1 1^(st) lens 38.30999265 6.690 plastic 1.650 21.40 97.151 2 89.51805989 2.123 3 2^(nd) lens 265.9237017 3.507 plastic 1.550 56.50 −10.831 4 5.817261412 18.739 5 Aperture plane −0.307 6 3^(rd) lens 26.13658896 2.057 plastic 1.565 58.00 21.399 7 −21.98589916 0.945 8 4^(th) lens 17.96887411 5.893 plastic 1.565 58.00 17.906 9 −20.55243477 1.029 10 5^(th) lens −18.88228376 1.448 plastic 1.632 23.40 −10.607 11 10.83179833 1.595 12 6^(th) lens 10.31720295 3.747 plastic 1.565 58.00 14.771 13 −38.56121899 4.786 14 7^(th) lens 11.26133857 6.137 plastic 1.565 58.00 54.802 15 14.18372014 0.800 16 Infrared plane 0.200 BK_7 1.517 64.2 rays filter 17 plane 0.610 18 Image plane plane Reference wavelength (d-line): 555 nm.

TABLE 4 Coefficients of the aspheric surfaces Surface 1 2 3 4 6 7 8 k 3.345583E−01 2.121547E+01 −7.965458E+00 −6.166041E−01 8.354258E+00 1.087213E+00 −5.968652E+00 A4 1.747694E−06 1.511633E−06 4.224255E−06 4.978518E−05 −1.085617E−04 −4.608874E−05 5.219771E−05 A6 −5.933480E−09 −9.423740E−09 −5.125456E−08 −5.834523E−07 −6.301166E−07 1.153742E−06 −9.195493E−07 A8 −1.796000E−11 −6.599000E−11 −8.886000E−11 −9.179410E−09 −1.434333E−08 −3.424057E−08 −1.447981E−08 A10 1.000000E−14 −1.000000E−14 4.700000E−13 −3.617700E−10 −4.921800E−10 −3.117000E−11 2.114000E−11 A12 0.000000E+00 0.000000E+00 0.000000E+00 0.000000E+00 0.000000E+00 0.000000E+00 0.000000E+00 A14 0.000000E+00 0.000000E+00 0.000000E+00 0.000000E+00 0.000000E+00 0.000000E+00 0.000000E+00 A16 0.000000E+00 0.000000E+00 0.000000E+00 0.000000E+00 0.000000E+00 0.000000E+00 0.000000E+00 Surface 9 10 11 12 13 14 15 k −4.521029E+01 −2.570506E+00 −1.506173E+01 −8.958277E+00 1.336178E+01 −4.018327E+00 −7.068737E+00 A4 −3.911505E−04 −1.441251E−04 4.381816E−05 −1.032315E−04 −2.563268E−04 −1.525988E−04 −7.181580E−04 A6 −3.278629E−06 −2.643422E−06 6.365011E−06 −8.750348E−07 3.153044E−06 −2.789229E−06 −1.462955E−06 A8 7.548049E−08 2.104616E−08 −1.895473E−07 1.276907E−08 −4.297162E−08 −3.954829E−08 6.996885E−08 A10 −4.067700E−10 6.022000E−10 1.610750E−09 −1.339900E−09 −3.634400E−10 −2.606700E−10 −4.298700E−10 A12 0.000000E+00 0.000000E+00 0.000000E+00 0.000000E+00 0.000000E+00 0.000000E+00 0.000000E+00 A14 0.000000E+00 0.000000E+00 0.000000E+00 0.000000E+00 0.000000E+00 0.000000E+00 0.000000E+00 A16 0.000000E+00 0.000000E+00 0.000000E+00 0.000000E+00 0.000000E+00 0.000000E+00 0.000000E+00

An equation of the aspheric surfaces of the second embodiment is the same as that of the first embodiment, and the definitions are the same as well.

The exact parameters of the second embodiment based on Table 3 and Table 4 are listed in the following table:

Second embodiment (Reference wavelength: 555 nm) |f/f1| |f/f2| |f/f3| |f/f4| |f/f5| |f/f6| 0.0722 0.6478 0.3278 0.3918 0.6614 0.4750 |f/f7| ΣPPR ΣNPR ΣPPR/|ΣNPR| IN12/f IN67/f 0.1280 1.3948 1.3092 1.0655 0.3026 0.6822 |f1/f2| |f2/f3| (TP1 + IN12)/TP2 (TP7 + IN67)/TP6 8.9701 0.5061 2.5128 2.9149 HOS InTL HOS/HOI InS/HOS ODT % TDT % 60.0000  58.3895  8.0000 0.4824 −2.0424  2.1042 HVT11 HVT12 HVT21 HVT22 HVT31 HVT32 0.0000 0.0000 11.7900  0.0000 0.0000 0.0000 HVT61 HVT62 HVT71 HVT72 HVT72/HOI HVT72/HOS 6.2440 0.0000 6.0491 4.4200 0.5893 0.0737 PSTA PLTA NSTA NLTA SSTA SLTA 0.014 mm 0.010 mm −0.001 mm −0.005 mm 0.005 mm 0.010 mm

The figures related to the profile curve lengths obtained based on Table 3 and Table 4 are listed in the following table:

Second embodiment (Reference wavelength: 555 nm) ARE ½(HEP) ARE value ARE − ½(HEP) 2(ARE/HEP) % TP ARE/TP (%) 11 2.506 2.507 0.00123 100.05% 6.690 37.47% 12 2.506 2.505 −0.00023  99.99% 6.690 37.45% 21 2.506 2.505 −0.00052  99.98% 3.507 71.43% 22 2.506 2.584 0.07869 103.14% 3.507 73.69% 31 2.506 2.509 0.00313 100.13% 2.057 121.97% 32 2.506 2.511 0.00508 100.20% 2.057 122.06% 41 2.506 2.513 0.00728 100.29% 5.893 42.64% 42 2.506 2.511 0.00537 100.21% 5.893 42.61% 51 2.506 2.513 0.00733 100.29% 1.448 173.54% 52 2.506 2.521 0.01552 100.62% 1.448 174.11% 61 2.506 2.524 0.01800 100.72% 3.747 67.35% 62 2.506 2.507 0.00180 100.07% 3.747 66.91% 71 2.506 2.523 0.01718 100.69% 6.137 41.11% 72 2.506 2.513 0.00772 100.31% 6.137 40.95% ARS EHD ARS value ARS − EHD (ARS/EHD) % TP ARS/TP (%) 11 19.321 20.159 0.838 104.34% 6.690 301.33% 12 16.688 16.787 0.099 100.59% 6.690 250.93% 21 15.308 15.312 0.004 100.03% 3.507 436.59% 22 8.227 11.517 3.290 139.99% 3.507 328.38% 31 5.963 5.996 0.034 100.57% 2.057 291.53% 32 6.119 6.224 0.105 101.72% 2.057 302.62% 41 6.901 7.005 0.104 101.51% 5.893 118.87% 42 7.163 7.508 0.345 104.82% 5.893 127.40% 51 6.763 6.992 0.229 103.38% 1.448 482.87% 52 6.799 6.969 0.170 102.50% 1.448 481.27% 61 7.050 7.156 0.106 101.50% 3.747 190.97% 62 7.425 7.773 0.348 104.69% 3.747 207.45% 71 7.275 7.423 0.148 102.04% 6.137 120.95% 72 8.189 8.573 0.384 104.68% 6.137 139.69%

The results of the equations of the second embodiment based on Table 3 and Table 4 are listed in the following table:

Values related to the inflection points of the second embodiment (Reference wavelength: 555 nm) HIF121 13.8715 HIF121/HOI 1.8495 SGI121 1.1718 |SGI121|/(|SGI121| + TP1) 0.1490 HIF211 8.0311 HIF211/HOI 1.0708 SGI211 0.1239 |SGI211|/(|SGI211| + TP2) 0.0341 HIF311 4.9399 HIF311/HOI 0.6586 SGI311 0.4310 |SGI311|/(|SGI311| + TP3) 0.1732 HIF411 5.6043 HIF411/HOI 0.7472 SGI411 0.7976 |SGI411|/(|SGI411| + TP4) 0.1192 HIF511 6.4678 HIF511/HOI 0.8624 SGI511 −1.3650 |SGI511|/(|SGI511| + TP5) 0.4853 HIF611 3.9563 HIF611/HOI 0.5275 SGI611 0.5843 |SGI611|/(|SGI611| + TP6) 0.1349 HIF711 3.8936 HIF711/HOI 0.5191 SGI711 0.5743 |SGI711|/(|SGI711| + TP7) 0.0856 HIF721 2.4948 HIF721/HOI 0.3326 SGI721 0.1819 |SGI721|/(|SGI721| + TP7) 0.0288

Third Embodiment

As shown in FIG. 3A and FIG. 3B, an optical image capturing system of the third embodiment of the present invention includes, along an optical axis from an object side to an image side, a first lens 310, an aperture 300, a second lens 320, a third lens 330, a fourth lens 340, a fifth lens 350, a sixth lens 360, a seventh lens 370, an infrared rays filter 380, an image plane 390, and an image sensor 392. FIG. 3C is a transverse aberration diagram at 0.7 field of view of the third embodiment of the present application.

The first lens 310 has positive refractive power and is made of plastic. An object-side surface 312 thereof, which faces the object side, is a convex aspheric surface, and an image-side surface 314 thereof, which faces the image side, is a concave aspheric surface. The image-side surface 314 has two inflection points.

The second lens 320 has negative refractive power and is made of plastic. An object-side surface 322 thereof, which faces the object side, is a convex aspheric surface, and an image-side surface 324 thereof, which faces the image side, is a concave aspheric surface. The object-side surface 322 and the image-side surface 324 both have an inflection point.

The third lens 330 has positive refractive power and is made of plastic. An object-side surface 332 thereof, which faces the object side, is a concave surface, and an image-side surface 334 thereof, which faces the image side, is a convex aspheric surface. The object-side surface 332 and the image-side surface 344 both have an inflection point.

The fourth lens 340 has positive refractive power and is made of plastic. An object-side surface 342, which faces the object side, is a concave aspheric surface, and an image-side surface 344, which faces the image side, is a convex aspheric surface. The object-side surface 342 has four inflection points, and the image-side surface 344 has an inflection point.

The fifth lens 350 has negative refractive power and is made of plastic. An object-side surface 352, which faces the object side, is a concave surface, and an image-side surface 354, which faces the image side, is a convex surface. The object-side surface 352 and the image-side surface 354 are both aspheric surface. The image-side surface 354 has an inflection point.

The sixth lens 360 has positive refractive power and is made of plastic. An object-side surface 362, which faces the object side, is a convex surface, and an image-side surface 364, which faces the image side, is a convex surface. The object-side surface 362 has three inflection points, and the image-side surface 364 has four inflection points. Whereby, incident angle of each field of view for the sixth lens can be effectively adjusted to improve aberration

The seventh lens 370 has negative refractive power and is made of plastic. An object-side surface 372, which faces the object side, is a concave surface, and an image-side surface 374, which faces the image side, is a concave surface. It may help to shorten the back focal length to keep small in size. In addition, the object-side surface 372 has two inflection points, and the image-side surface 374 has an inflection point, which may reduce an incident angle of the light of an off-axis field of view and correct the aberration of the off-axis field of view.

The infrared rays filter 380 is made of glass and between the seventh lens 370 and the image plane 390. The infrared rays filter 390 gives no contribution to the focal length of the system.

In the third embodiment, the optical image capturing system of the third embodiment further satisfies ΣPP=57.1785 mm; and f1/ΣPP=0.2408, where ΣPP is a sum of the focal lengths of each positive lens. It is helpful to share the positive refractive power of one single lens to other positive lenses to avoid the significant aberration caused by the incident rays.

The optical image capturing system of the third embodiment further satisfies ΣNP=−53.3826 mm; and f2/ΣNP =0.1153, where ΣNP is a sum of the focal lengths of each negative lens. It is helpful to share the negative refractive power of the sixth lens 360 to other negative lenses.

The parameters of the lenses of the third embodiment are listed in Table 5 and Table 6.

TABLE 5 f = 9.5423 mm; f/HEP = 2.0; HAF = 38.0002 deg Focal Thickness Refractive Abbe length Surface Radius of curvature (mm) (mm) Material index number (mm) 0 Object plane infinity 1 1^(st) lens 5.126953214 1.214 plastic 1.544 55.96 13.7691 2 14.77967651 0.259 3 Aperture plane 0.570 4 2^(nd) lens 7.744320593 0.542 plastic 1.642 22.46 −18.6536 5 4.589392077 0.440 6 3^(rd) lens −27.72740863 0.922 plastic 1.544 55.96 16.899 7 −7.003148313 0.126 8 4^(th) lens −132.5407952 1.087 plastic 1.544 55.96 16.6825 9 −8.545788217 1.661 10 5^(th) lens −2.747454197 0.790 plastic 1.642 22.46 −28.5748 11 −3.590917294 0.100 12 6^(th) lens 6.331804041 1.192 plastic 1.544 55.96 9.82793 13 −32.79464874 1.173 14 7^(th) lens −5.604046294 0.602 plastic 1.544 55.96 −6.15416 15 8.705420907 0.465 16 Infrared plane 0.300 BK_7 1.517 64.2 rays filter 17 plane 1.300 18 Image plane 0.000 plane Reference wavelength (d-line): 555 nm.

TABLE 6 Coefficients of the aspheric surfaces Surface 1 2 4 5 6 7 8 k −1.064649E+00 −7.156630E+00 −8.946824E+01 8.010624E−01 1.357282E+01 −9.621586E−01 4.656054E+01 A4 1.358278E−03 −3.143285E−03 3.689773E−04 −1.972531E−02 3.856100E−03 1.072596E−02 1.070986E−02 A6 −1.537317E−04 8.407030E−04 −1.086803E−02 −5.320992E−04 −2.894203E−03 −8.790456E−03 −7.964556E−03 A8 1.520498E−04 −1.133322E−04 5.229602E−03 8.331800E−04 7.813465E−04 3.233125E−03 2.848458E−03 A10 −4.144138E−05 −1.780766E−05 −1.496221E−03 −2.811037E−04 −2.147279E−04 −7.174150E−04 −5.716041E−04 A12 6.312734E−06 1.361900E−05 2.595275E−04 5.079297E−05 4.021990E−05 9.754134E−05 6.824275E−05 A14 −4.305616E−07 −2.475022E−06 −2.472214E−05 −4.585964E−06 −3.710161E−06 −7.750199E−06 −4.621737E−06 A16 8.866670E−09 1.459490E−07 9.370067E−07 1.561873E−07 1.333560E−07 2.738341E−07 1.338013E−07 Surface 9 10 11 12 13 14 15 k −1.506072E+01 −8.908616E−01 −4.153787E−01 −1.440067E+00 2.345828E+01 −2.975038E−02 −3.905794E−01 A4 −2.328261E−03 2.514134E−02 1.533485E−02 −1.483034E−02 −1.243722E−02 −5.870219E−03 −4.473415E−03 A6 −1.112969E−03 −8.683162E−03 −3.976145E−03 2.862703E−03 3.059330E−03 1.800358E−03 3.399395E−04 A8 3.524178E−04 1.770667E−03 6.061738E−04 −3.832590E−04 −3.034689E−04 −1.981376E−04 −2.491328E−05 A10 −6.261380E−05 −2.367895E−04 −5.731690E−05 3.232370E−05 1.366570E−05 1.226012E−05 1.188238E−06 A12 9.114956E−06 2.032129E−05 3.435847E−06 −1.903324E−06 −2.484401E−07 −4.283668E−07 −3.419726E−08 A14 −8.301954E−07 −1.025564E−06 −1.227677E−07 6.751249E−08 1.089800E−10 7.951930E−09 5.339600E−10 A16 2.944219E−08 2.270383E−08 2.016940E−09 −1.007020E−09 3.193000E−11 −6.085000E−11 −3.490000E−12

An equation of the aspheric surfaces of the third embodiment is the same as that of the first embodiment, and the definitions are the same as well.

The exact parameters of the third embodiment based on Table 5 and Table 6 are listed in the following table:

Third embodiment (Reference wavelength: 555 nm) |f/f1| |f/f2| |f/f3| |f/f4| |f/f5| |f/f6| 0.6930 0.5116 0.5647 0.5720 0.3339 0.9709 |f/f7| ΣPPR ΣNPR ΣPPR/|ΣNPR| IN12/f IN67/f 1.5505 2.8006 2.3960 1.1689 0.0869 0.1229 |f1/f2| |f2/f3| (TP1 + IN12)/TP2 (TP7 + IN67)/TP6 0.7381 1.1038 3.7730 1.4898 HOS InTL HOS/HOI InS/HOS ODT % TDT % 12.7407  10.6762  1.6988 0.8844 1.0235 0.4634 HVT11 HVT12 HVT21 HVT22 HVT31 HVT32 0.0000 0.0000 1.3043 2.0996 2.7393 0.0000 HVT61 HVT62 HVT71 HVT72 HVT72/HOI HVT72/HOS 2.7964 4.7698 0.0000 4.0398 0.5386 0.3171 PSTA PLTA NSTA NLTA SSTA SLTA −0.002 mm −0.024 mm −0.006 mm −0.002 mm 0.005 mm −0.005 mm

The figures related to the profile curve lengths obtained based on Table 5 and Table 6 are listed in the following table:

Third embodiment (Reference wavelength: 555 nm) ARE ARE − 2(ARE/ ARE/TP ARE 1/2(HEP) value 1/2(HEP) HEP) % TP (%) 11 2.386 2.494 0.109 104.56% 1.214 205.43% 12 2.385 2.392 0.006 100.27% 1.214 196.97% 21 2.356 2.392 0.037 101.57% 0.542 441.71% 22 2.386 2.397 0.012 100.48% 0.542 442.57% 31 2.386 2.397 0.012 100.49% 0.922 260.05% 32 2.386 2.447 0.062 102.59% 0.922 265.49% 41 2.386 2.385 −0.001 99.98% 1.087 219.47% 42 2.386 2.425 0.040 101.67% 1.087 223.19% 51 2.386 2.586 0.201 108.42% 0.790 327.59% 52 2.386 2.515 0.129 105.41% 0.790 318.49% 61 2.386 2.397 0.012 100.49% 1.192 201.19% 62 2.386 2.394 0.008 100.34% 1.192 200.89% 71 2.386 2.463 0.077 103.24% 0.602 409.02% 72 2.386 2.398 0.012 100.52% 0.602 398.25% ARS ARS − (ARS/ ARS/TP ARS EHD value EHD EHD) % TP (%) 11 2.765 2.963 0.198 107.15% 1.214 244.00% 12 2.385 2.392 0.006 100.27% 1.214 196.97% 21 2.356 2.392 0.037 101.57% 0.542 441.71% 22 2.765 2.783 0.018 100.65% 0.542 513.79% 31 2.818 2.833 0.015 100.55% 0.922 307.32% 32 2.921 3.079 0.157 105.39% 0.922 333.95% 41 3.145 3.183 0.038 101.21% 1.087 292.88% 42 3.300 3.468 0.169 105.12% 1.087 319.17% 51 3.400 4.161 0.761 122.37% 0.790 527.00% 52 3.872 4.603 0.731 118.87% 0.790 582.97% 61 4.452 4.708 0.256 105.75% 1.192 395.15% 62 5.029 5.095 0.065 101.30% 1.192 427.58% 71 5.228 5.510 0.282 105.39% 0.602 915.04% 72 6.419 6.728 0.310 104.83% 0.602 1117.46%

The results of the equations of the third embodiment based on Table 5 and Table 6 are listed in the following table:

Values related to the inflection points of the third embodiment (Reference wavelength: 555 nm) HIF121 2.3213 HIF121/HOI 0.3095 SGI121 0.1503 |SGI121|/(|SGI121| + TP1) 0.1102 HIF122 2.3596 HIF122/HOI 0.3146 SGI122 0.1549 |SGI122|/(|SGI122| + TP1) 0.1132 HIF211 0.7262 HIF211/HOI 0.0968 SGI211 0.0280 |SGI211|/(|SGI211| + TP2) 0.0492 HIF221 1.0711 HIF221/HOI 0.1428 SGI221 0.1024 |SGI221|/(|SGI221| + TP2) 0.1591 HIF311 2.2817 HIF311/HOI 0.3042 SGI311 −0.1592 |SGI311|/(|SGI311| + TP3) 0.1473 HIF321 2.7143 HIF321/HOI 0.3619 SGI321 −0.6623 |SGI321|/(|SGI321| + TP3) 0.4181 HIF411 0.2581 HIF411/HOI 0.0344 SGI411 −0.0002 |SGI411|/(|SGI411| + TP4) 0.0002 HIF412 0.9763 HIF412/HOI 0.1302 SGI412 0.0012 |SGI412|/(|SGI412| + TP4) 0.0011 HIF413 1.6099 HIF413/HOI 0.2147 SGI413 0.0025 |SGI413|/(|SGI413| + TP4) 0.0023 HIF414 2.1553 HIF414/HOI 0.2874 SGI414 0.0041 |SGI414|/(|SGI414| + TP4) 0.0038 HIF421 3.1927 HIF421/HOI 0.4257 SGI421 −0.7812 |SGI421|/(|SGI421| + TP4) 0.4182 HIF521 3.8199 HIF521/HOI 0.5093 SGI521 −2.0739 |SGI521|/(|SGI521| + TP5) 0.7243 HIF611 1.5835 HIF611/HOI 0.2111 SGI611 0.1362 |SGI611|/(|SGI611| + TP6) 0.1026 HIF612 4.0634 HIF612/HOI 0.5418 SGI612 −0.2673 |SGI612|/(|SGI612| + TP6) 0.1833 HIF613 4.3009 HIF613/HOI 0.5735 SGI613 −0.4534 |SGI613|/(|SGI613| + TP6) 0.2756 HIF621 1.8405 HIF621/HOI 0.2454 SGI621 −0.1107 |SGI621|/(|SGI621| + TP6) 0.0850 HIF622 2.6284 HIF622/HOI 0.3505 SGI622 −0.1977 |SGI622|/(|SGI622| + TP6) 0.1423 HIF623 3.9646 HIF623/HOI 0.5286 SGI623 −0.4724 |SGI623|/(|SGI623| + TP6) 0.2839 HIF624 4.9355 HIF624/HOI 0.6581 SGI624 −0.6399 |SGI624|/(|SGI624| + TP6) 0.3494 HIF711 3.4061 HIF711/HOI 0.4541 SGI711 −0.9805 |SGI711|/(|SGI711| + TP7) 0.6196 HIF712 5.0056 HIF712/HOI 0.6674 SGI712 −1.5615 |SGI712|/(|SGI712| + TP7) 0.7217 HIF721 2.0478 HIF721/HOI 0.2730 SGI721 0.1830 |SGI721|/(|SGI721| + TP7) 0.2331

Fourth Embodiment

As shown in FIG. 4A and FIG. 4B, an optical image capturing system 40 of the fourth embodiment of the present invention includes, along an optical axis from an object side to an image side, a first lens 410, an aperture 400, a second lens 420, a third lens 430, a fourth lens 440, a fifth lens 450, a sixth lens 460, a seventh lens 470, an infrared rays filter 480, an image plane 490, and an image sensor 492. FIG. 4C is a transverse aberration diagram at 0.7 field of view of the fourth embodiment of the present application.

The first lens 410 has positive refractive power and is made of plastic. An object-side surface 412 thereof, which faces the object side, is a convex aspheric surface, and an image-side surface 414 thereof, which faces the image side, is a concave aspheric surface. The image-side surface 414 has two inflection points.

The second lens 420 has negative refractive power and is made of plastic. An object-side surface 422 thereof, which faces the object side, is a convex aspheric surface, and an image-side surface 424 thereof, which faces the image side, is a concave aspheric surface. The object-side surface 422 and the image-side surface 424 both have an inflection point.

The third lens 430 has positive refractive power and is made of plastic. An object-side surface 432 thereof, which faces the object side, is a convex aspheric surface, and an image-side surface 434 thereof, which faces the image side, is a convex aspheric surface. The object-side surface 432 has two inflection points, and the image-side surface 434 has an inflection point.

The fourth lens 440 has positive refractive power and is made of plastic. An object-side surface 442, which faces the object side, is a concave aspheric surface, and an image-side surface 444, which faces the image side, is a convex aspheric surface. The image-side surface 444 has an inflection point.

The fifth lens 450 has negative refractive power and is made of plastic. An object-side surface 452, which faces the object side, is a concave aspheric surface, and an image-side surface 454, which faces the image side, is a convex aspheric surface. The image-side surface 454 has two inflection points.

The sixth lens 660 has positive refractive power and is made of plastic. An object-side surface 462, which faces the object side, is a convex surface, and an image-side surface 464, which faces the image side, is a convex surface. The object-side surface 462 and the image-side surface 464 both have two inflection points. Whereby, incident angle of each field of view for the sixth lens can be effectively adjusted to improve aberration.

The seventh lens 470 has negative refractive power and is made of plastic. An object-side surface 472, which faces the object side, is a concave surface, and an image-side surface 474, which faces the image side, is a concave surface. It may help to shorten the back focal length to keep small in size. In addition, the object-side surface 472 has an inflection point, which may reduce an incident angle of the light of an off-axis field of view and correct the aberration of the off-axis field of view.

The infrared rays filter 480 is made of glass and between the seventh lens 470 and the image plane 490. The infrared rays filter 480 gives no contribution to the focal length of the system.

In the fourth embodiment, the optical image capturing system of the fourth embodiment further satisfies ΣPP=56.0883 mm; and f1/ΣPP=0.2233, where ΣPP is a sum of the focal lengths of each positive lens. It is helpful to share the positive refractive power of one single lens to other positive lenses to avoid the significant aberration caused by the incident rays.

The optical image capturing system of the fourth embodiment further satisfies ΣNP=−87.3758 mm; and f2/ΣNP =0.0585, where ΣNP is a sum of the focal lengths of each negative lens. It is helpful to share the negative refractive power of the sixth lens 460 to other negative lenses.

The parameters of the lenses of the fourth embodiment are listed in Table 7 and Table 8.

TABLE 7 f = 6.8656 mm; f/HEP = 1.8; HAF = 47.5 deg Focal Thickness Refractive Abbe length Surface Radius of curvature (mm) (mm) Material index number (mm) 0 Object plane infinity 1 1^(st) lens 3.601476359 0.889 plastic 1.544 55.96 12.5245 2 6.947158259 0.307 3 Aperture plane 0.100 4 2^(nd) lens 5.276720377 0.300 plastic 1.642 22.46 −55.9514 5 4.503058022 0.136 6 3^(rd) lens 24.443000967 0.709 plastic 1.544 55.96 12.9402 7 −9.832995605 0.443 8 4^(th) lens −126.659175869 0.515 plastic 1.544 55.96 23.8412 9 −11.818661867 0.599 10 5^(th) lens −1.830314760 0.982 plastic 1.642 22.46 −26.3112 11 −2.483182141 0.100 12 6^(th) lens 5.693008556 1.579 plastic 1.544 55.96 6.78244 13 −9.551309876 0.815 14 7^(th) lens −5.217815016 0.617 plastic 1.584 29.89 −5.11316 15 7.387853451 0.366 16 Infrared plane 0.300 BK_7 1.517 64.2 rays filter 17 plane 1.000 18 Image plane 0.000 plane Reference wavelength (d-line): 587.5 nm; the position of blocking light: blocking at the first surface with effective semi diameter of 2.320 mm; blocking at the fifth surface with effective semi diameter of 1.750 mm.

TABLE 8 Coefficients of the aspheric surfaces Surface 1 2 4 5 6 7 8 k −4.218427E−01 −2.641534E+00 −1.943524E+01 −2.576642E+00 −2.638477E+01  1.251815E+01  9.917239E+01 A4  1.374568E−03 −5.169524E−03 −9.552506E−03 −9.694420E−03  8.274332E−03 −9.269063E−03 −2.539792E−02 A6 −6.187329E−04 −6.014409E−04 −8.655393E−03 −4.272939E−03  1.471004E−03 −1.423521E−03 −2.476999E−03 A8  3.172341E−04  3.498418E−04  1.341537E−03  4.846662E−04 −8.675639E−04  1.056495E−03 −4.752220E−04 A10 −1.043248E−04 −1.170928E−04  5.822625E−04  1.935885E−04 −2.908188E−04 −8.021186E−05 −1.249185E−05 A12  1.690748E−05  1.916946E−05 −1.543434E−04 −6.594969E−05  9.661237E−05 −1.073785E−04  7.141822E−06 A14 −1.990841E−06 −9.902798E−08  7.303311E−07  9.554668E−08 −1.766522E−06  2.465907E−05 −7.021694E−06 A16  1.404622E−07 −1.655272E−07 −1.355712E−07 −1.419891E−07  1.558800E−07  6.551488E−07  1.829315E−06 Surface 9 10 11 12 13 14 15 k  2.140866E+01 −4.130031E−01 −5.748779E−01 −1.634525E+00 −6.477384E+01 −4.553673E−02 −1.567468E+01 A4 −1.193827E−02  3.003641E−02  8.447238E−03 −9.657550E−03 −8.148340E−03 −4.300000E−03 −4.269638E−03 A6 −3.482473E−03 −6.618354E−03 −2.302313E−03  1.669624E−03  2.904242E−03  1.571107E−03  4.118127E−04 A8  1.403202E−04  1.440880E−03  5.287956E−04 −2.163588E−04 −3.847761E−04 −1.638559E−04 −2.883837E−05 A10 −4.040280E−05 −6.554964E−05 −4.570815E−05  1.257647E−05  2.475592E−05  9.853622E−06  1.306841E−06 A12  2.163276E−06  6.752684E−06  3.520462E−06 −3.655210E−07 −8.498852E−07 −3.369603E−07 −3.623542E−08 A14 −7.821445E−07 −2.888837E−06 −1.694344E−07  6.481140E−09  1.494319E−08  5.988200E−09  5.516300E−10 A16  5.380421E−07  6.060977E−07 −2.000000E−11 −7.324000E−11 −1.065200E−10 −4.124000E−11 −3.560000E−12

An equation of the aspheric surfaces of the fourth embodiment is the same as that of the first embodiment, and the definitions are the same as well.

The exact parameters of the fourth embodiment based on Table 7 and Table 8 are listed in the following table:

Fourth embodiment (Reference wavelength: 555 nm) |f/f1| |f/f2| |f/f3| |f/f4| |f/f5| |f/f6| 0.5482 0.1227 0.5306 0.2880 0.2609 1.0123 |f/f7| ΣPPR ΣNPR ΣPPR/|ΣNPR| IN12/f IN67/f 1.3427 2.3790 1.7264 1.3780 0.0592 0.1187 |f1/f2| |f2/f3| (TP1 + IN12)/TP2 (TP7 + IN67)/TP6 0.2238 4.3238 4.3185 0.9072 HOS InTL HOS/HOI InS/HOS ODT % TDT % 9.7580 8.0922 1.3011 0.8775 2.5000 2.4000 HVT11 HVT12 HVT21 HVT22 HVT31 HVT32 0.0000 0.0000 1.2678 1.5900 0.0000 0.0000 HVT61 HVT62 HVT71 HVT72 HVT72/HOI HVT72/HOS 2.8404 0.0000 0.0000 3.5321 0.4710 0.3620 PSTA PLTA NSTA NLTA SSTA SLTA −0.062 mm 0.012 mm −0.016 mm −0.019 mm 0.009 mm 0.013 mm

The figures related to the profile curve lengths obtained based on Table 7 and Table 8 are listed in the following table:

Fourth embodiment (Reference wavelength: 555 nm) ARE ARE − 2(ARE/ ARE/TP ARE 1/2(HEP) value 1/2(HEP) HEP) % TP (%) 11 1.907 2.003 0.096 105.02% 0.889 225.30% 12 1.907 1.917 0.010 100.53% 0.889 215.66% 21 1.745 1.751 0.007 100.38% 0.300 583.75% 22 1.750 1.759 0.009 100.53% 0.300 586.44% 31 1.822 1.827 0.004 100.24% 0.709 257.71% 32 1.907 1.941 0.034 101.78% 0.709 273.81% 41 1.907 2.079 0.172 109.00% 0.515 403.42% 42 1.907 2.030 0.123 106.45% 0.515 393.96% 51 1.907 2.181 0.274 114.37% 0.982 222.03% 52 1.907 2.072 0.165 108.63% 0.982 210.89% 61 1.907 1.925 0.017 100.91% 1.579 121.88% 62 1.907 1.915 0.007 100.39% 1.579 121.25% 71 1.907 1.953 0.045 102.38% 0.617 316.33% 72 1.907 1.915 0.008 100.42% 0.617 310.28% ARS ARS − (ARS/ ARS/TP ARS EHD value EHD EHD) % TP (%) 11 2.320 2.487 0.167 107.20% 0.889 279.77% 12 2.041 2.052 0.011 100.53% 0.889 230.84% 21 1.745 1.751 0.007 100.38% 0.300 583.75% 22 1.750 1.759 0.009 100.53% 0.300 586.44% 31 1.822 1.827 0.004 100.24% 0.709 257.71% 32 1.922 1.955 0.033 101.72% 0.709 275.79% 41 1.973 2.191 0.219 111.10% 0.515 425.27% 42 2.207 2.492 0.285 112.92% 0.515 483.63% 51 2.276 2.721 0.445 119.55% 0.982 276.93% 52 3.040 3.414 0.374 112.32% 0.982 347.53% 61 4.556 4.712 0.156 103.41% 1.579 298.40% 62 4.986 5.304 0.318 106.38% 1.579 335.89% 71 5.207 5.535 0.328 106.29% 0.617 896.77% 72 6.441 6.811 0.370 105.74% 0.617 1103.43% 

The results of the equations of the fourth embodiment based on Table 7 and Table 8 are listed in the following table:

Values related to the inflection points of the fourth embodiment (Reference wavelength: 555 nm) HIF121 1.3972 HIF121/HOI 0.1863 SGI121 0.1168 |SGI121|/(|SGI121| + TP1) 0.1162 HIF122 1.9644 HIF122/HOI 0.2619 SGI122 0.1889 |SGI122|/(|SGI122| + TP1) 0.1752 HIF211 0.7306 HIF211/HOI 0.0974 SGI211 0.0429 |SGI211|/(|SGI211| + TP2) 0.1250 HIF221 0.9819 HIF221/HOI 0.1309 SGI221 0.0928 |SGI221|/(|SGI221| + TP2) 0.2363 HIF311 1.4063 HIF311/HOI 0.1875 SGI311 0.0669 |SGI311|/(|SGI311| + TP3) 0.0863 HIF312 1.6254 HIF312/HOI 0.2167 SGI312 0.0894 |SGI312|/(|SGI312| + TP3) 0.1120 HIF321 1.6900 HIF321/HOI 0.2253 SGI321 −0.2345 |SGI321|/(|SGI321| + TP3) 0.2486 HIF421 2.1180 HIF421/HOI 0.2824 SGI421 −0.7420 |SGI421|/(|SGI421| + TP4) 0.5902 HIF521 2.1477 HIF521/HOI 0.2864 SGI521 −0.8933 |SGI521|/(|SGI521| + TP5) 0.4762 HIF522 2.9216 HIF522/HOI 0.3895 SGI522 −1.3728 |SGI522|/(|SGI522| + TP5) 0.5829 HIF611 1.8402 HIF611/HOI 0.2454 SGI611 0.2234 |SGI611|/(|SGI611| + TP6) 0.1239 HIF612 3.9456 HIF612/HOI 0.5261 SGI612 0.0074 |SGI612|/(|SGI612| + TP6) 0.0047 HIF621 1.4937 HIF621/HOI 0.1992 SGI621 −0.1064 |SGI621|/(|SGI621| + TP6) 0.0631 HIF622 2.5164 HIF622/HOI 0.3355 SGI622 −0.2040 |SGI622|/(|SGI622| + TP6) 0.1144 HIF711 2.5652 HIF711/HOI 0.3420 SGI711 −0.6203 |SGI711|/(|SGI711| + TP7) 0.5012 HIF712 4.3050 HIF712/HOI 0.5740 SGI712 −1.2247 |SGI712|/(|SGI712| + TP7) 0.6649 HIF721 1.4814 HIF721/HOI 0.1975 SGI721 0.1146 |SGI721|/(|SGI721| + TP7) 0.1565

Fifth Embodiment

As shown in FIG. 5A and FIG. 5B, an optical image capturing system of the fifth embodiment of the present invention includes, along an optical axis from an object side to an image side, a first lens 510, a second lens 520, a third lens 530, an aperture 500, a fourth lens 540, a fifth lens 550, a sixth lens 560, a seventh lens 570, an infrared rays filter 580, an image plane 590, and an image sensor 592. FIG. 5C is a transverse aberration diagram at 0.7 field of view of the fifth embodiment of the present application.

The first lens 510 has positive refractive power and is made of plastic. An object-side surface 512, which faces the object side, is a convex aspheric surface, and an image-side surface 514, which faces the image side, is a concave aspheric surface.

The second lens 520 has negative refractive power and is made of plastic. An object-side surface 522 thereof, which faces the object side, is a convex aspheric surface, and an image-side surface 524 thereof, which faces the image side, is a concave aspheric surface. The image-side surface 524 has an inflection point.

The third lens 530 has positive refractive power and is made of plastic. An object-side surface 532, which faces the object side, is a convex aspheric surface, and an image-side surface 534, which faces the image side, is a concave aspheric surface.

The fourth lens 540 has positive refractive power and is made of plastic. An object-side surface 542, which faces the object side, is a concave aspheric surface, and an image-side surface 544, which faces the image side, is a convex aspheric surface.

The fifth lens 550 has positive refractive power and is made of plastic. An object-side surface 552, which faces the object side, is a convex aspheric surface, and an image-side surface 554, which faces the image side, is a convex aspheric surface. The object-side surface 552 has an inflection point.

The sixth lens 560 can have positive refractive power and is made of plastic. An object-side surface 562, which faces the object side, is a convex surface, and an image-side surface 564, which faces the image side, is a convex surface. The object-side surface 562 has two inflection points, and the image-side surface 564 has an inflection point. Whereby, incident angle of each field of view for the sixth lens 560 can be effectively adjusted to improve aberration.

The seventh lens 570 has negative refractive power and is made of plastic. An object-side surface 572, which faces the object side, is a concave surface, and an image-side surface 574, which faces the image side, is a convex surface. It may help to shorten the back focal length to keep small in size. In addition, the object-side surface 572 and the image-side surface 574 both have an inflection point, which may reduce an incident angle of the light of an off-axis field of view and correct the aberration of the off-axis field of view.

The infrared rays filter 580 is made of glass and between the seventh lens 570 and the image plane 590. The infrared rays filter 580 gives no contribution to the focal length of the system.

In the fifth embodiment, the optical image capturing system of the fifth embodiment further satisfies ΣPP=178.9037 mm; and f1/ΣPP=0.4233, where ΣPP is a sum of the focal lengths of each positive lens. It is helpful to share the positive refractive power of one single lens to other positive lenses to avoid the significant aberration caused by the incident rays.

The optical image capturing system of the fifth embodiment further satisfies ΣNP=−41.0270 mm; and f7/ΣNP =0.7332, where ΣNP is a sum of the focal lengths of each negative lens. It is helpful to share the negative refractive power of one single lens to other negative lenses.

The parameters of the lenses of the fifth embodiment are listed in Table 9 and Table 10.

TABLE 9 f = 6.7437 mm; f/HEP = 1.2; HAF = 47.4980 deg Focal Radius of curvature Thickness Refractive Abbe length Surface (mm) (mm) Material index number (mm) 0 Object plane infinity 1 1^(st) lens 38.41549872 3.083 plastic 1.650 21.40 75.725 2 164.5702173 0.051 3 2^(nd) lens 25.05742058 1.828 plastic 1.514 56.80 −10.923 4 4.484579084 1.422 5 3^(rd) lens 7.747689137 4.336 plastic 1.650 21.40 48.146 6 7.993162782 1.838 7 Aperture plane 0.660 8 4^(th) lens −28.36730639 5.531 plastic 1.565 58.00 15.401 9 −7.145672538 0.116 10 5^(th) lens 18.70637432 5.689 plastic 1.565 58.00 15.622 11 −14.96142417 1.411 12 6^(th) lens 14.99356494 5.269 plastic 1.565 58.00 24.011 13 −128.6124653 1.108 14 7^(th) lens −15.50208128 0.673 plastic 1.650 21.40 −30.104 15 −73.56363056 0.700 16 Infrared plane 0.200 BK_7 1.517 64.2 rays filter 17 plane 1.085 18 Image plane plane Reference wavelength (d-line): 555 nm.

TABLE 10 Coefficients of the aspheric surfaces Surface 1 2 3 4 5 6 8 k −1.516714E+00 3.374432E+01 1.818263E+00 −6.750988E−01 −2.849603E−01 3.933454E+00 3.860484E+01 A4 1.595233E−05 1.684952E−05 −3.775903E−05 −9.580167E−05 −5.691900E−05 2.051521E−04 −3.259130E−04 A6 −4.019400E−10 7.312610E−09 1.329275E−07 −5.194715E−06 9.286641E−07 1.985735E−05 −7.981440E−06 A8 −3.420000E−12 7.920000E−11 3.386200E−10 −9.256678E−08 6.189397E−08 2.853734E−07 −1.012572E−06 A10 −1.600000E−13 4.800000E−13 6.250000E−12 −1.423600E−09 1.543630E−09 −5.527219E−08 9.907847E−08 A12 0.000000E+00 0.000000E+00 3.000000E−14 −2.774000E−11 2.586000E−11 2.995300E−09 7.424600E−09 A14 0.000000E+00 0.000000E+00 0.000000E+00 0.000000E+00 −4.300000E−13 9.873100E−10 −3.558300E−10 A16 0.000000E+00 0.000000E+00 0.000000E+00 0.000000E+00 0.000000E+00 0.000000E+00 0.000000E+00 Surface 9 10 11 12 13 14 15 k 2.380207E−01 −1.960669E+00 −2.123206E+00 −4.403179E+00 3.356474E+01 2.175100E+00 2.296751E+01 A4 −2.839258E−04 −2.349293E−05 4.885172E−05 −2.214845E−04 −1.475931E−04 9.883455E−05 1.851032E−04 A6 −6.140481E−06 −2.272014E−08 −1.121620E−07 −4.434699E−08 −1.930089E−06 2.233778E−07 7.070317E−07 A8 2.575404E−08 7.875300E−10 −3.165880E−09 5.862920E−09 −1.477393E−08 9.015100E−10 −1.216596E−08 A10 1.171000E−10 −3.042000E−11 −2.164000E−11 1.318900E−10 −8.832000E−11 6.273000E−11 1.844300E−10 A12 −7.053000E−11 −3.800000E−13 −1.000000E−14 1.420000E−12 4.380000E−12 −1.600000E−13 −6.780000E−12 A14 −3.270000E−12 0.000000E+00 0.0000000E+00 0.000000E+00 6.000000E−14 7.000000E−14 2.500000E−13 A16 0.000000E+00 0.000000E+00 0.000000E+00 0.000000E+00 0.000000E+00 0.000000E+00 0.000000E+00

An equation of the aspheric surfaces of the fifth embodiment is the same as that of the first embodiment, and the definitions are the same as well.

The exact parameters of the fifth embodiment based on Table 9 and Table 10 are listed in the following table:

Fifth embodiment (Reference wavelength: 555 nm) |f/f1| |f/f2| |f/f3| |f/f4| |f/f5| |f/f6| 0.0891 0.6174 0.1401 0.4379 0.4317 0.2809 |f/f7| ΣPPR ΣNPR ΣPPR/|ΣNPR| IN12/f IN67/f 0.2240 1.3796 0.8414 1.6396 0.0076 0.1643 |f1/f2| |f2/f3| (TP1 + IN12)/TP2 (TP7 + IN67)/TP6 6.9326 0.2269 1.7147 0.3379 HOS InTL HOS/HOI InS/HOS ODT % TDT % 35.0000  33.0149  4.6667 0.6412 2.4971 0.4277 HVT11 HVT12 HVT21 HVT22 HVT31 HVT32 0.0000 0.0000 0.0000 0.0000 0.0000 0.0000 HVT61 HVT62 HVT71 HVT72 HVT72/HOI HVT72/HOS 0.0000 0.0000 0.0000 4.2248 0.5633 0.1207 PSTA PLTA NSTA NLTA SSTA SLTA −0.055 mm 0.020 mm 0.043 mm −0.056 mm −0.090 mm 0.073 mm

The figures related to the profile curve lengths obtained based on Table 9 and Table 10 are listed in the following table:

Fifth embodiment (Reference wavelength: 555 nm) ARE ½(HEP) ARE value ARE − ½(HEP) 2(ARE/HEP) % TP ARE/TP (%) 11 2.810 2.812 0.00169 100.06% 3.083 91.18% 12 2.810 2.809 −0.00072 99.97% 3.083 91.10% 21 2.810 2.815 0.00493 100.18% 1.828 153.99% 22 2.810 2.993 0.18271 106.50% 1.828 163.71% 31 2.810 2.872 0.06229 102.22% 4.336 66.23% 32 2.810 2.912 0.10205 103.63% 4.336 67.15% 41 2.810 2.818 0.00769 100.27% 5.531 50.94% 42 2.810 2.896 0.08578 103.05% 5.531 52.35% 51 2.810 2.819 0.00935 100.33% 5.689 49.55% 52 2.810 2.825 0.01474 100.52% 5.689 49.65% 61 2.810 2.822 0.01252 100.45% 5.269 53.57% 62 2.810 2.809 −0.00042 99.99% 5.269 53.32% 71 2.810 2.824 0.01454 100.52% 0.673 419.90% 72 2.810 2.809 −0.00048 99.98% 0.673 417.67% ARS EHD ARS value ARS − EHD (ARS/EHD)% TP ARS/TP (%) 11 15.182 15.789 0.607 104.00% 3.083 512.07% 12 14.305 14.523 0.218 101.52% 3.083 471.00% 21 11.632 12.469 0.836 107.19% 1.828 682.11% 22 7.059 9.202 2.143 130.36% 1.828 503.40% 31 6.771 8.393 1.622 123.96% 4.336 193.54% 32 3.580 4.175 0.594 116.60% 4.336 96.27% 41 3.811 3.840 0.029 100.77% 5.531 69.42% 42 5.711 7.347 1.636 128.65% 5.531 132.83% 51 8.148 8.326 0.178 102.18% 5.689 146.34% 52 8.462 8.797 0.335 103.96% 5.689 154.63% 61 8.293 8.417 0.124 101.50% 5.269 159.75% 62 7.714 7.858 0.144 101.87% 5.269 149.14% 71 7.528 7.842 0.314 104.17% 0.673 1165.89% 72 7.224 7.275 0.051 100.71% 0.673 1081.55%

The results of the equations of the fifth embodiment based on Table 9 and Table 10 are listed in the following table:

Values related to the inflection points of the fifth embodiment (Reference wavelength: 555 nm) HIF121 2.3213 HIF121/HOI 0.3095 SGI121 0.1503 |SGI121|/(|SGI121| + TP1) 0.1102 HIF122 2.3596 HIF122/HOI 0.3146 SGI122 0.1549 |SGI122|/(|SGI122| + TP1) 0.1132 HIF211 0.7262 HIF211/HOI 0.0968 SGI211 0.0280 |SGI211|/(|SGI211| + TP2) 0.0492 HIF221 1.0711 HIF221/HOI 0.1428 SGI221 0.1024 |SGI221|/(|SGI221| + TP2) 0.1591 HIF311 2.2817 HIF311/HOI 0.3042 SGI311 −0.1592 |SGI311|/(|SGI311| + TP3) 0.1473 HIF321 2.7143 HIF321/HOI 0.3619 SGI321 −0.6623 |SGI321|/(|SGI321| + TP3) 0.4181 HIF411 0.2581 HIF411/HOI 0.0344 SGI411 −0.0002 |SGI411|/(|SGI411| + TP4) 0.0002 HIF412 0.9763 HIF412/HOI 0.1302 SGI412 0.0012 |SGI412|/(|SGI412| + TP4) 0.0011 HIF413 1.6099 HIF413/HOI 0.2147 SGI413 0.0025 |SGI413|/(|SGI413| + TP4) 0.0023 HIF414 2.1553 HIF414/HOI 0.2874 SGI414 0.0041 |SGI414|/(|SGI414| + TP4) 0.0038 HIF421 3.1927 HIF421/HOI 0.4257 SGI421 −0.7812 |SGI421|/(|SGI421| + TP4) 0.4182 HIF521 3.8199 HIF521/HOI 0.5093 SGI521 −2.0739 |SGI521|/(|SGI521| + TP5) 0.7243 HIF611 1.5835 HIF611/HOI 0.2111 SGI611 0.1362 |SGI611|/(|SGI611| + TP6) 0.1026 HIF612 4.0634 HIF612/HOI 0.5418 SGI612 −0.2673 |SGI612|/(|SGI612| + TP6) 0.1833 HIF613 4.3009 HIF613/HOI 0.5735 SGI613 −0.4534 |SGI613|/(|SGI613| + TP6) 0.2756 HIF621 1.8405 HIF621/HOI 0.2454 SGI621 −0.1107 |SGI621|/(|SGI621| + TP6) 0.0850 HIF622 2.6284 HIF622/HOI 0.3505 SGI622 −0.1977 |SGI622|/(|SGI622| + TP6) 0.1423 HIF623 3.9646 HIF623/HOI 0.5286 SGI623 −0.4724 |SGI623|/(|SGI623| + TP6) 0.2839 HIF624 4.9355 HIF624/HOI 0.6581 SGI624 −0.6399 |SGI624|/(|SGI624| + TP6) 0.3494 HIF711 3.4061 HIF711/HOI 0.4541 SGI711 −0.9805 |SGI711|/(|SGI711| + TP7) 0.6196 HIF712 5.0056 HIF712/HOI 0.6674 SGI712 −1.5615 |SGI712|/(|SGI712| + TP7) 0.7217 HIF721 2.0478 HIF721/HOI 0.2730 SGI721 0.1830 |SGI721|/(|SGI721| + TP7) 0.2331

Sixth Embodiment

As shown in FIG. 6A and FIG. 6B, an optical image capturing system of the sixth embodiment of the present invention includes, along an optical axis from an object side to an image side, a first lens 610, an aperture 600, a second lens 620, a third lens 630, a fourth lens 640, a fifth lens 650, a seventh lens 660, a seventh lens 670, an infrared rays filter 680, an image plane 690, and an image sensor 692. FIG. 6C is a transverse aberration diagram at 0.7 field of view of the sixth embodiment of the present application.

The first lens 610 has positive refractive power and is made of plastic. An object-side surface 612, which faces the object side, is a convex aspheric surface, and an image-side surface 614, which faces the image side, is a convex aspheric surface. The object-side surface 612 has an inflection point.

The second lens 620 has negative refractive power and is made of plastic. An object-side surface 622 thereof, which faces the object side, is a convex aspheric surface, and an image-side surface 624 thereof, which faces the image side, is a concave aspheric surface. The object-side surface 622 and the image-side surface 624 both have an inflection point.

The third lens 630 has positive refractive power and is made of plastic. An object-side surface 632, which faces the object side, is a convex aspheric surface, and an image-side surface 634, which faces the image side, is a convex aspheric surface. The object-side surface 632 has an inflection point.

The fourth lens 640 has positive refractive power and is made of plastic. An object-side surface 642, which faces the object side, is a convex aspheric surface, and an image-side surface 644, which faces the image side, is a convex aspheric surface. The object-side surface 642 has two inflection points.

The fifth lens 650 has negative refractive power and is made of plastic. An object-side surface 652, which faces the object side, is a concave aspheric surface, and an image-side surface 654, which faces the image side, is a convex aspheric surface. The object-side surface 652 and the image-side surface 654 both have two inflection points.

The sixth lens 660 can have positive refractive power and is made of plastic. An object-side surface 662, which faces the object side, is a convex surface, and an image-side surface 664, which faces the image side, is a convex surface. The object-side surface 662 has two inflection points, and the image-side surface 664 has three inflection points. Whereby, incident angle of each field of view for the sixth lens 660 can be effectively adjusted to improve aberration.

The seventh lens 670 has negative refractive power and is made of plastic. An object-side surface 672, which faces the object side, is a concave surface, and an image-side surface 674, which faces the image side, is a convex surface. It may help to shorten the back focal length to keep small in size. In addition, it may reduce an incident angle of the light of an off-axis field of view and correct the aberration of the off-axis field of view.

The infrared rays filter 680 is made of glass and between the seventh lens 670 and the image plane 690. The infrared rays filter 680 gives no contribution to the focal length of the system.

In the sixth embodiment, the optical image capturing system of the sixth embodiment further satisfies ΣPP=62.7420 mm; and f1/ΣPP=0.2381, where ΣPP is a sum of the focal lengths of each positive lens. It is helpful to share the positive refractive power of one single lens to other positive lenses to avoid the significant aberration caused by the incident rays.

The optical image capturing system of the sixth embodiment further satisfies Σ/NP=−88.6984 mm; and f7/ΣNP=0.0806, where ΣNP is a sum of the focal lengths of each negative lens. It is helpful to share the negative refractive power of one single lens to the other negative lenses to avoid the significant aberration caused by the incident rays.

The parameters of the lenses of the sixth embodiment are listed in Table 11 and Table 12.

TABLE 11 f = 6.830 mm; f/HEP = 1.6; HAF = 47.5 deg Focal Radius of curvature Thickness Refractive Abbe length Surface (mm) (mm) Material index number (mm) 0 Object plane infinity 1 1^(st) lens 22.92669222 0.782 plastic 1.544 55.96 14.940 2 −12.50533563 0.101 3 Aperture plane 0.100 4 2^(nd) lens 3.414733165 0.400 plastic 1.642 22.46 −27.654 5 2.735872028 0.627 6 3^(rd) lens 25.0700232 1.114 plastic 1.544 55.96 26.746 7 −34.41000821 0.210 8 4^(th) lens 89.20096062 1.274 plastic 1.544 55.96 14.495 9 −8.638595141 0.560 10 5^(th) lens −2.047917945 0.689 plastic 1.642 22.46 −53.900 11 −2.463255196 0.100 12 6^(th) lens 6.29780764 1.101 plastic 1.544 55.96 6.562 13 −7.792827475 0.100 14 7^(th) lens 1.817247142 0.403 plastic 1.642 22.46 −7.145 15 1.191109992 1.139 16 Infrared plane 0.300 BK_7 1.517 64.2 rays filter 17 plane 2.100 18 Image plane 0.000 plane Reference wavelength (d-line): 555 nm; the position of blocking light: blocking at the first surface with effective semi diameter of 2.200 mm; blocking at the seventh surface with effective semi diameter of 2.275 mm.

TABLE 12 Coefficients of the aspheric surfaces Surface 1 2 4 5 6 7 8 k 8.519837E+01 −9.000000E+01 −3.351396E+00 −9.397617E−01 −1.916083E+01 3.401159E+01 9.000000E+01 A4 2.374462E−03 −5.838686E−03 −2.291764E−02 −3.213095E−02 −2.459788E−03 −2.687800E−02 −3.504567E−02 A6 −1.612226E−03 4.395112E−03 9.276993E−03 7.779255E−03 7.321283E−04 8.896301E−03 1.368358E−02 A8 5.288473E−04 −2.200633E−03 −4.200876E−03 −2.129420E−03 −2.008436E−03 −6.128646E−03 −8.251017E−03 A10 −1.576862E−04 6.372117E−04 1.117507E−03 1.850027E−04 1.142530E−03 2.252164E−03 2.801748E−03 A12 3.075118E−05 −1.149037E−04 −1.799793E−04 5.218940E−05 −3.532551E−04 −4.656386E−04 −5.316745E−04 A14 −3.944190E−06 1.062391E−05 1.162220E−05 −1.954396E−05 5.267700E−05 5.089052E−05 5.254294E−05 A16 1.933549E−07 −3.588671E−07 2.716061E−07 1.982470E−06 −3.502449E−06 −2.347679E−06 −2.052826E−06 Surface 9 10 11 12 13 14 15 k −2.670809E+01 −5.682341E−01 −6.598428E−01 −2.726292E+00 −9.000000E+01 −5.542566E+00 −3.272144E+00 A4 −3.836182E−02 −2.612266E−02 −1.049654E−02 9.782575E−03 3.354961E−02 2.468524E−03 −6.836340E−03 A6 9.267657E−03 2.022422E−02 8.397277E−03 −1.182916E−03 −4.676770E−03 −2.596987E−03 −3.917020E−04 A8 −2.459905E−03 −5.248210E−03 −1.737698E−03 −1.797794E−05 2.884197E−04 3.240621E−04 8.533027E−05 A10 4.634531E−04 8.507499E−04 2.058819E−04 6.239689E−06 −8.287770E−06 −1.834018E−05 −5.100116E−06 A12 −5.102977E−05 −7.181237E−05 −1.044135E−05 −2.938476E−07 4.544651E−08 5.321956E−07 1.467939E−07 A14 2.681167E−06 2.426471E−06 4.487730E−08 5.833340E−09 2.555930E−09 −7.576070E−09 −2.082250E−09 A16 −4.196504E−08 4.307730E−09 8.094270E−09 −4.375000E−11 −3.796000E−11 4.053000E−11 1.160000E−11

An equation of the aspheric surfaces of the sixth embodiment is the same as that of the first embodiment, and the definitions are the same as well.

The exact parameters of the sixth embodiment based on Table 11 and Table 12 are listed in the following table:

Sixth embodiment (Reference wavelength: 555 nm) |f/f1| |f/f2| |f/f3| |f/f4| |f/f5| |f/f6| 0.4572 0.2470 0.2554 0.4712 0.1267 1.0409 |f/f7| ΣPPR ΣNPR ΣPPR/|ΣNPR| IN12/f IN67/f 0.9560 2.2248 1.3297 1.6731 0.0295 0.0146 |f1/f2| |f2/f3| (TP1 + IN12)/TP2 (TP7 + IN67)/TP6 0.5402 1.0340 2.4583 0.4566 HOS InTL HOS/HOI InS/HOS ODT % TDT % 11.1019  7.5625 1.4803 0.9204 2.0054 1.3214 HVT11 HVT12 HVT21 HVT22 HVT31 HVT32 2.1665 0.0000 1.9156 0.0000 1.3729 0.0000 HVT61 HVT62 HVT71 HVT72 HVT72/HOI HVT72/HOS 3.2480 0.0000 2.8232 3.4670 0.4623 0.3123 PSTA PLTA NSTA NLTA SSTA SLTA −0.005 mm 0.024 mm 0.022 mm 0.010 mm −0.006 mm 0.023 mm

The figures related to the profile curve lengths obtained based on Table 11 and Table 12 are listed in the following table:

Sixth embodiment (Reference wavelength: 555 nm) ARE ½(HEP) ARE value ARE − ½(HEP) 2(ARE/HEP) % TP ARE/TP (%) 11 2.134 2.137 0.002 100.11% 0.782 273.25% 12 2.134 2.147 0.012 100.57% 0.782 274.50% 21 2.074 2.097 0.022 101.08% 0.400 524.19% 22 2.087 2.131 0.044 102.09% 0.400 532.75% 31 2.093 2.128 0.035 101.65% 1.114 190.98% 32 2.134 2.264 0.129 106.05% 1.114 203.18% 41 2.134 2.236 0.101 104.74% 1.274 175.44% 42 2.134 2.274 0.140 106.55% 1.274 178.47% 51 2.134 2.427 0.293 113.71% 0.689 352.28% 52 2.134 2.333 0.198 109.30% 0.689 338.60% 61 2.134 2.194 0.060 102.81% 1.101 199.24% 62 2.134 2.163 0.028 101.32% 1.101 196.35% 71 2.134 2.224 0.089 104.18% 0.403 552.01% 72 2.134 2.306 0.172 108.04% 0.403 572.47% ARS EHD ARS value ARS − EHD (ARS/EHD) % TP ARS/TP (%) 11 2.200 2.202 0.002 100.09% 0.782 281.56% 12 2.159 2.173 0.013 100.61% 0.782 277.82% 21 2.074 2.097 0.022 101.08% 0.400 524.19% 22 2.087 2.131 0.044 102.09% 0.400 532.75% 31 2.093 2.128 0.035 101.65% 1.114 190.98% 32 2.275 2.478 0.203 108.94% 1.114 222.44% 41 2.389 2.571 0.182 107.63% 1.274 201.77% 42 2.778 3.214 0.436 115.68% 1.274 252.20% 51 2.943 3.308 0.364 112.38% 0.689 480.06% 52 3.270 3.534 0.264 108.07% 0.689 512.97% 61 4.936 5.088 0.152 103.08% 1.101 461.95% 62 5.271 5.575 0.304 105.76% 1.101 506.16% 71 5.414 5.630 0.216 103.99% 0.403 1397.59%  72 5.895 6.197 0.301 105.11% 0.403 1538.22% 

The results of the equations of the sixth embodiment based on Table 11 and Table 12 are listed in the following table:

Values related to the inflection points of the sixth embodiment (Reference wavelength: 555 nm) HIF111 1.6856 HIF111/HOI 0.2247 SGI111 0.0702 |SGI111|/(|SGI111| + TP1) 0.0823 HIF211 1.1663 HIF211/HOI 0.1555 SGI211 0.1579 |SGI211|/(|SGI211| + TP2) 0.2830 HIF221 1.2636 HIF221/HOI 0.1685 SGI221 0.2310 |SGI221|/(|SGI221| + TP2) 0.3661 HIF311 0.8985 HIF311/HOI 0.1198 SGI311 0.0142 |SGI311|/(|SGI311| + TP3) 0.0126 HIF411 0.1655 HIF411/HOI 0.0221 SGI411 0.0001 |SGI411|/(|SGI411| + TP4) 0.0001 HIF412 2.2930 HIF412/HOI 0.3057 SGI412 −0.5927 |SGI412|/(|SGI412| + TP4) 0.3175 HIF511 1.7740 HIF511/HOI 0.2365 SGI511 −0.7862 |SGI511|/(|SGI511| + TP5) 0.5329 HIF512 2.8492 HIF512/HOI 0.3799 SGI512 −1.3557 |SGI512|/(|SGI512| + TP5) 0.6630 HIF521 1.8793 HIF521/HOI 0.2506 SGI521 −0.6944 |SGI521|/(|SGI521| + TP5) 0.5019 HIF522 3.2152 HIF522/HOI 0.4287 SGI522 −1.0509 |SGI522|/(|SGI522| + TP5) 0.6040 HIF611 2.1327 HIF611/HOI 0.2844 SGI611 0.4380 |SGI611|/(|SGI611| + TP6) 0.2845 HIF612 4.1144 HIF612/HOI 0.5486 SGI612 0.5361 |SGI612|/(|SGI612| + TP6) 0.3274 HIF621 0.4745 HIF621/HOI 0.0633 SGI621 −0.0118 |SGI621|/(|SGI621| + TP6) 0.0106 HIF622 2.3646 HIF622/HOI 0.3153 SGI622 0.2918 |SGI622|/(|SGI622| + TP6) 0.2094 HIF623 5.0158 HIF623/HOI 0.6688 SGI623 0.0632 |SGI623|/(|SGI623| + TP6) 0.0543 HIF711 1.2844 HIF711/HOI 0.1713 SGI711 0.3205 |SGI711|/(|SGI711| + TP7) 0.4431 HIF721 1.2208 HIF721/HOI 0.1628 SGI721 0.4244 |SGI721|/(|SGI721| + TP7) 0.5131

Seventh Embodiment

As shown in FIG. 7A and FIG. 7B, an optical image capturing system of the seventh embodiment of the present invention includes, along an optical axis from an object side to an image side, a first lens 710, a second lens 720, a third lens 730, an aperture 700, a fourth lens 740, a fifth lens 750, a seventh lens 760, a seventh lens 770, an infrared rays filter 780, an image plane 790, and an image sensor 792. FIG. 7C is a transverse aberration diagram at 0.7 field of view of the seventh embodiment of the present application.

The first lens 710 has positive refractive power and is made of plastic. An object-side surface 712, which faces the object side, is a convex aspheric surface, and an image-side surface 714, which faces the image side, is a concave aspheric surface. The object-side surface 712 and image-side surface 714 both have an inflection point.

The second lens 720 has negative refractive power and is made of plastic. An object-side surface 722 thereof, which faces the object side, is a convex aspheric surface, and an image-side surface 724 thereof, which faces the image side, is a concave aspheric surface. The object-side surface 722 and the image-side surface 724 both have an inflection point.

The third lens 730 has positive refractive power and is made of plastic. An object-side surface 732, which faces the object side, is a convex aspheric surface, and an image-side surface 734, which faces the image side, is a concave aspheric surface. The object-side surface 732 and the image-side surface 734 both have an inflection point.

The fourth lens 740 has positive refractive power and is made of plastic. An object-side surface 742, which faces the object side, is a concave aspheric surface, and an image-side surface 744, which faces the image side, is a convex aspheric surface. The object-side surface 742 has an inflection point.

The fifth lens 750 has negative refractive power and is made of plastic. An object-side surface 752, which faces the object side, is a convex aspheric surface, and an image-side surface 754, which faces the image side, is a concave aspheric surface. The object-side surface 752 and the image-side surface 754 both have two inflection points.

The sixth lens 760 can have positive refractive power and is made of plastic.

An object-side surface 762, which faces the object side, is a convex surface, and an image-side surface 764, which faces the image side, is a concave surface. The object-side surface 762 has two inflection points, and the image-side surface 764 has an inflection point. Whereby, incident angle of each field of view for the sixth lens 760 can be effectively adjusted to improve aberration.

The seventh lens 770 has negative refractive power and is made of plastic. An object-side surface 772, which faces the object side, is a concave surface, and an image-side surface 774, which faces the image side, is a concave surface. It may help to shorten the back focal length to keep small in size. In addition, it may reduce an incident angle of the light of an off-axis field of view and correct the aberration of the off-axis field of view.

The infrared rays filter 780 is made of glass and between the seventh lens 770 and the image plane 790. The infrared rays filter 780 gives no contribution to the focal length of the system.

In the seventh embodiment, the optical image capturing system of the seventh embodiment further satisfies ΣPP=74.3451 mm; and f1/ΣPP=0.3344, where ΣPP is a sum of the focal lengths of each positive lens. It is helpful to share the positive refractive power of one single lens to other positive lenses to avoid the significant aberration caused by the incident rays.

The optical image capturing system of the seventh embodiment further satisfies ΣNP=−4865.9186 mm; and f7/ΣNP=0.0013, where ΣNP is a sum of the focal lengths of each negative lens. It is helpful to share the negative refractive power of one single lens to the other negative lenses to avoid the significant aberration caused by the incident rays.

The parameters of the lenses of the sixth embodiment are listed in Table 13 and Table 14.

TABLE 13 f = 7.9627 mm; f/HEP = 1.2; HAF = 42.4993 deg Focal Radius of Thickness Refractive Abbe length Surface curvature (mm) (mm) Material index number (mm) 0 Object plane infinity 1 1^(st) lens 23.25741102 4.194 plastic 1.650 21.40 38.852 2 249.1225869 0.756 3 2^(nd) lens 35.33386893 1.380 plastic 1.565 58.00 −11.031 4 5.237191673 5.183 5 3^(rd) lens 9.353367306 1.633 plastic 1.550 56.50 16.751 6 −731.5920373 0.050 7 Aperture plane 1.265 8 4^(th) lens −4.269794289 1.539 plastic 1.650 21.40 −21.345 9 −7.022091895 0.050 10 5^(th) lens 26.01930755 5.494 plastic 1.565 58.00 14.184 11 −10.74451776 0.050 12 6^(th) lens 13.31994285 6.926 plastic 1.565 58.00 14.119 13 −16.27410602 3.385 14 7^(th) lens −8.075088802 0.870 plastic 1.650 21.40 −25.888 15 −16.06479743 0.300 16 Infrared plane 0.200 BK_7 1.517 64.2 rays filter 17 plane 1.725 18 Image plane plane Reference wavelength (d-line): 555 nm.

TABLE 14 Coefficients of the aspheric surfaces Surface 1 2 4 5 6 7 8 k 7.259491E−01 5.000000E+01 7.032207E+00 −9.630902E−01   9.539991E−01 −5.000000E+01  −2.096807E−01 A4 6.063994E−05 2.538166E−04 −5.645850E−05  5.076614E−04 −2.373762E−04 −5.368718E−04   4.498802E−03 A6 3.106379E−07 1.510051E−06 8.820465E−06 9.249612E−07 −1.167773E−05 8.509966E−06 −1.075804E−05 A8 7.037070E−09 3.273984E−08 2.274920E−08 8.824704E−07  2.041107E−06 4.016836E−07 −7.841815E−07 A10 1.847000E−11 4.391000E−10 −1.917400E−09  2.278497E−08 −1.142338E−08 4.836128E−08  2.845209E−08 A12 −6.900000E−13  −9.580000E−12  6.620000E−12 −1.100840E−09  −9.736380E−09 −7.583460E−09   5.708490E−09 A14 0.000000E+00 7.000000E−14 4.000000E−14 5.460000E−12  4.516600E−10 4.220200E−10 −3.092000E−11 A16 0.000000E+00 0.000000E+00 0.000000E+00 0.000000E+00  0.000000E+00 0.000000E+00  0.000000E+00 Surface 9 10 11 12 13 14 15 k −3.552125E+00 −4.737869E+01  4.928003E−01 4.371738E−01 −1.987535E+01 −8.551448E−02  −2.740577E+00 A4  1.783222E−03 −3.512530E−04 −3.205531E−04 8.511538E−05  4.739271E−05 1.851742E−04  5.330067E−04 A6  1.129836E−05  9.947697E−06  4.753289E−06 −1.481707E−06  −1.077151E−06 2.069437E−06  6.847817E−06 A8 −5.336123E−07 −2.123288E−07 −6.764542E−08 7.641320E−09 −3.657354E−08 3.531386E−08 −1.156630E−09 A10 −4.851400E−10 −2.454310E−09 −1.715400E−09 −1.624100E−10  −1.223200E−10 3.904100E−10 −1.582240E−09 A12 −2.190000E−11  2.976600E−10  2.994000E−11 −1.920000E−12   1.138000E−11 −2.621000E−11  −2.478000E−11 A14 −2.750000E−12 −4.760000E−12 −6.000000E−14 5.000000E−14 −3.000000E−14 3.600000E−13  5.600000E−13 A16  0.000000E+00  0.000000E+00  0.000000E+00 0.000000E+00  0.000000E+00 0.000000E+00  0.000000E+00

An equation of the aspheric surfaces of the seventh embodiment is the same as that of the first embodiment, and the definitions are the same as well.

The exact parameters of the seventh embodiment based on Table 13 and Table 14 are listed in the following table:

Seventh embodiment (Reference wavelength: 555 nm) |f/f1| |f/f2| |f/f3| |f/f4| |f/f5| |f/f6| 0.2050 0.7218 0.4754 0.3731 0.5614 0.5640 |f/f7| ΣPPR ΣNPR ΣPPR/|ΣNPR| IN12/f IN67/f 0.3076 1.8057 1.4025 1.2875 0.0949 0.4251 |f1/f2| |f2/f3| (TP1 + IN12)/TP2 (TP7 + IN67)/TP6 3.5220 0.6586 3.5876 0.6143 HOS InTL HOS/HOI InS/HOS ODT % TDT % 35.0000  32.7755  4.6667 0.6230 2.5133 0.4529 HVT11 HVT12 HVT21 HVT22 HVT31 HVT32 0.0000 0.0000 0.0000 0.0000 0.0000 3.7153 HVT61 HVT62 HVT71 HVT72 HVT72/HOI HVT72/HOS 0.0000 0.0000 0.0000 4.5521 0.6069 0.1301 PSTA PLTA NSTA NLTA SSTA SLTA 0.017 mm −0.010 mm −0.038 mm −0.019 mm −0.006 mm 0.020 mm

The figures related to the profile curve lengths obtained based on Table 13 and Table 14 are listed in the following table:

Seventh embodiment (Reference wavelength: 555 nm) 1/ ARE ARE − 2(ARE/ ARE/ ARE 2(HEP) value 1/2(HEP) HEP) % TP TP (%) 11 3.318 3.329 0.01161 100.35% 4.194 79.38% 12 3.318 3.318 0.00008 100.00% 4.194 79.10% 21 3.318 3.323 0.00478 100.14% 1.380 240.79% 22 3.318 3.566 0.24794 107.47% 1.380 258.41% 31 3.318 3.390 0.07247 102.18% 1.633 207.62% 32 3.318 3.318 −0.00001 100.00% 1.633 203.18% 41 3.318 3.480 0.16189 104.88% 1.539 226.16% 42 3.318 3.356 0.03796 101.14% 1.539 218.11% 51 3.318 3.321 0.00324 100.10% 5.494 60.44% 52 3.318 3.383 0.06474 101.95% 5.494 61.56% 61 3.318 3.355 0.03680 101.11% 6.926 48.43% 62 3.318 3.332 0.01465 100.44% 6.926 48.11% 71 3.318 3.409 0.09113 102.75% 0.870 391.67% 72 3.318 3.330 0.01179 100.36% 0.870 382.55% ARS ARS − (ARS/ ARS/ ARS EHD value EHD EHD)% TP TP (%) 11 10.400 11.407 1.007 109.68% 4.194 271.96% 12 8.049 8.815 0.765 109.51% 4.194 210.15% 21 7.736 8.130 0.393 105.08% 1.380 589.15% 22 5.154 6.460 1.306 125.34% 1.380 468.18% 31 4.315 4.525 0.210 104.86% 1.633 277.11% 32 4.119 4.122 0.003 100.06% 1.633 252.41% 41 4.074 4.294 0.221 105.42% 1.539 279.11% 42 4.978 5.029 0.051 101.03% 1.539 326.88% 51 5.859 5.866 0.007 100.11% 5.494 106.76% 52 6.912 8.052 1.140 116.50% 5.494 146.56% 61 8.445 9.268 0.823 109.74% 6.926 133.80% 62 7.859 7.998 0.139 101.77% 6.926 115.48% 71 6.508 7.148 0.640 109.83% 0.870 821.27% 72 6.720 6.799 0.079 101.18% 0.870 781.16%

The results of the equations of the seventh embodiment based on Table 13 and Table 14 are listed in the following table.

Values related to the inflection points of the seventh embodiment (Reference wavelength: 555 nm) HIF211 8.0110 HIF211/HOI 1.0681 SGI211 2.0751 |SGI211|/(|SGI211| + TP2) 0.6006 HIF321 3.1408 HIF321/HOI 0.4188 SGI321 −0.0456 |SGI321|/(|SGI321| + TP3) 0.0272 HIF411 3.0619 HIF411/HOI 0.4082 SGI411 −0.8540 |SGI411|/(|SGI411| + TP4) 0.3569 HIF421 2.1505 HIF421/HOI 0.2867 SGI421 −0.2726 |SGI421|/(|SGI421| + TP4) 0.1505 HIF511 2.7916 HIF511/HOI 0.3722 SGI511 0.1164 |SGI511|/(|SGI511| + TP5) 0.0207 HIF621 7.1043 HIF621/HOI 0.9472 SGI621 −1.1205 |SGI621|/(|SGI621| + TP6) 0.1392 HIF721 2.7163 HIF721/HOI 0.3622 SGI721 −0.1951 |SGI721|/(|SGI721| + TP7) 0.1831

Eighth Embodiment

As shown in FIG. 8A and FIG. 8B, an optical image capturing system of the eighth embodiment of the present invention includes, along an optical axis from an object side to an image side, a first lens 810, a second lens 820, a third lens 830, an aperture 800, a fourth lens 840, a fifth lens 850, a seventh lens 860, a seventh lens 870, an infrared rays filter 880, an image plane 890, and an image sensor 892. FIG. 8C is a transverse aberration diagram at 0.7 field of view of the eighth embodiment of the present application.

The first lens 810 has positive refractive power and is made of plastic. An object-side surface 812, which faces the object side, is a concave aspheric surface, and an image-side surface 814, which faces the image side, is a convex aspheric surface. The object-side surface 812 and image-side surface 814 both have an inflection point.

The second lens 820 has negative refractive power and is made of plastic. An object-side surface 822 thereof, which faces the object side, is a convex aspheric surface, and an image-side surface 824 thereof, which faces the image side, is a concave aspheric surface.

The third lens 830 has positive refractive power and is made of plastic. An object-side surface 832, which faces the object side, is a convex aspheric surface, and an image-side surface 834, which faces the image side, is a concave aspheric surface. The object-side surface 832 and the image-side surface 834 both have an inflection point.

The fourth lens 840 has negative refractive power and is made of plastic. An object-side surface 842, which faces the object side, is a concave aspheric surface, and an image-side surface 844, which faces the image side, is a convex aspheric surface. The object-side surface 842 and the image-side surface 844 both have an inflection point.

The fifth lens 850 has positive refractive power and is made of plastic. An object-side surface 852, which faces the object side, is a convex aspheric surface, and an image-side surface 854, which faces the image side, is a convex aspheric surface. The object-side surface 852 has two inflection points.

The sixth lens 860 can have positive refractive power and is made of plastic. An object-side surface 862, which faces the object side, is a concave surface, and an image-side surface 864, which faces the image side, is a convex surface. The object-side surface 862 and the image-side surface 864 both have an inflection point. Whereby, incident angle of each field of view for the sixth lens 860 can be effectively adjusted to improve aberration.

The seventh lens 870 has negative refractive power and is made of plastic. An object-side surface 872, which faces the object side, is a concave surface, and an image-side surface 874, which faces the image side, is a concave surface. The image-side surface 874 has two inflection points. It may help to shorten the back focal length to keep small in size. In addition, it may reduce an incident angle of the light of an off-axis field of view and correct the aberration of the off-axis field of view.

The infrared rays filter 880 is made of glass and between the seventh lens 870 and the image plane 890. The infrared rays filter 880 gives no contribution to the focal length of the system.

In the eighth embodiment, the optical image capturing system of the seventh embodiment further satisfies ΣPP=80.7833 mm; and f1/ΣPP=0.3779, where ΣPP is a sum of the focal lengths of each positive lens. It is helpful to share the positive refractive power of one single lens to other positive lenses to avoid the significant aberration caused by the incident rays.

The optical image capturing system of the eighth embodiment further satisfies ΣNP=−138.2578 mm; and f7/ΣNP =0.0605, where ΣNP is a sum of the focal lengths of each negative lens. It is helpful to share the negative refractive power of one single lens to the other negative lenses to avoid the significant aberration caused by the incident rays.

The parameters of the lenses of the sixth embodiment are listed in Table 15 and Table 16.

TABLE 15 f = 8.1614 mm; f/HEP = 1.2; HAF = 42.5004 deg Focal Radius of curvature Thickness Refractive Abbe length Surface (mm) (mm) Material index number (mm) 0 Object plane plane 1 1^(st) lens −10.49584781 6.025 plastic 1.565 58.00 30.531 2 −7.889849611 0.050 3 2^(nd) lens 6.202752831 1.682 1.650 21.40 −100.000 4 5.057989171 0.631 plastic 5 3^(rd) lens 8.240060359 1.212 1.514 56.80 24.901 6 21.84929863 0.068 plastic 7 Aperture plane 0.629 8 4^(th) lens −6.108818989 0.488 plastic 1.650 21.40 −29.889 9 −9.157845181 0.326 10 5^(th) lens 20.67646082 3.348 plastic 1.565 58.00 12.640 11 −10.32046019 1.729 12 6^(th) lens −176.4958843 0.903 plastic 1.565 58.00 12.712 13 −6.934869515 2.265 14 7^(th) lens −8.974395123 0.802 plastic 1.650 21.40 −8.369 15 14.60939939 0.800 16 Infrared plane 0.200 BK_7 1.517 64.2 rays filter 17 plane 0.347 18 Image plane plane Reference wavelength (d-line): 555 nm.

TABLE 16 Coefficients of the aspheric surfaces Surface 1 2 3 4 5 6 8 k −7.207639E+00 −8.299802E+00 −2.006712E+00 2.810153E−02 7.219310E−02 2.524126E+01 −8.361677E+00 A4 1.787113E−05 3.826449E−05 −2.135562E−04 −3.588632E−03 1.037320E−03 −1.204794E−03 2.089626E−03 A6 1.852201E−07 1.050240E−06 3.067715E−05 1.644906E−04 −5.241587E−05 −9.277654E−05 −4.819963E−07 A8 5.486010E−09 3.223270E−09 −9.728463E−07 −1.408052E−06 2.694087E−06 1.860634E−06 −1.817734E−06 A10 −4.623000E−11 7.792500E−10 4.669697E−08 −1.070802E−07 8.063412E−08 9.902109E−08 3.982788E−08 A12 −1.500000E−13 −2.228000E−11 2.497100E−09 6.637670E−09 −6.673010E−09 −2.374540E−09 8.887230E−09 A14 0.000000E+00 1.400000E−13 −7.056000E−11 1.204990E−09 −5.121100E−10 −4.034000E−11 −4.539000E−11 A16 0.000000E+00 0.000000E+00 0.000000E+00 0.000000E+00 0.000000E+00 0.000000E+00 0.000000E+00 Surface 9 10 11 12 13 14 15 k −1.996249E+01 2.317494E+01 −2.880295E+00 −5.000000E+01 −3.731277E+00 1.196856E+00 −5.000000E+01 A4 3.783662E−03 −1.570957E−03 −1.788279E−03 −7.011103E−04 3.908411E−04 −1.217226E−03 −8.358329E−04 A6 2.054378E−05 −2.582997E−05 −2.522595E−05 −8.941617E−06 −1.004588E−05 2.950368E−05 −6.544913E−06 A8 9.686901E−07 2.275732E−07 −7.370659E−07 −6.887843E−07 6.892740E−09 3.805125E−07 −3.514799E−08 A10 1.722921E−08 −4.870903E−08 2.987693E−08 −2.363911E−08 −5.878780E−09 −1.304821E−08 5.793900E−10 A12 −3.364610E−09 −3.479600E−10 7.504700E−10 3.593000E−11 −5.409800E−10 −6.474500E−10 2.020000E−11 A14 −1.502100E−10 2.279800E−10 −1.249300E−10 7.625000E−11 5.881000E−11 6.510000E−12 6.100000E−13 A16 0.000000E+00 0.000000E+00 0.000000E+00 0.000000E+00 0.000000E+00 0.000000E+00 0.000000E+00

An equation of the aspheric surfaces of the eighth embodiment is the same as that of the first embodiment, and the definitions are the same as well.

The exact parameters of the eighth embodiment based on Table 15 and Table 16 are listed in the following table:

Eighth embodiment (Reference wavelength: 555 nm) |f/f1| |f/f2| |f/f3| |f/f4| |f/f5| |f/f6| 0.2673 0.0816 0.3278 0.2731 0.6457 0.6421 |f/f7| ΣPPR ΣNPR ΣPPR/|ΣNPR| IN12/f IN67/f 0.9752 1.8828 1.3299 1.4158 0.0061 0.2775 |f1/f2| |f2/f3| (TP1 + IN12)/TP2 (TP7 + IN67)/TP6 0.3053 4.0159 3.6111 3.3971 HOS InTL HOS/HOI InS/HOS ODT % TDT % 21.5042  20.1580  2.8672 0.5504 −2.5351  2.5339 HVT11 HVT12 HVT21 HVT22 HVT31 HVT32 0.0000 0.0000 0.0000 0.0000 0.0000 2.7625 HVT61 HVT62 HVT71 HVT72 HVT72/HOI HVT72/HOS 0.0000 0.0000 0.0000 3.1667 0.4222 0.1473 PSTA PLTA NSTA NLTA SSTA SLTA 0.043 mm −0.007 mm −0.021 mm −0.035 mm 0.004 mm 0.022 mm

The figures related to the profile curve lengths obtained based on Table 15 and Table 16 are listed in the following table:

Eighth embodiment (Reference wavelength: 555 nm) ARE − ARE ½(HEP) ARE value ½(HEP) 2(ARE/HEP) % TP ARE/TP (%) 11 3.401 3.442 0.042 101.23% 6.025  57.13% 12 3.401 3.458 0.058 101.69% 6.025  57.40% 21 3.401 3.547 0.146 104.29% 1.682 210.81% 22 3.401 3.631 0.230 106.77% 1.682 215.82% 31 3.401 3.537 0.137 104.02% 1.212 291.97% 32 3.401 3.403 0.002 100.06% 1.212 280.85% 41 3.401 3.429 0.028 100.84% 0.488 702.13% 42 3.401 3.437 0.037 101.07% 0.488 703.77% 51 3.401 3.403 0.002 100.06% 3.348 101.63% 52 3.401 3.548 0.147 104.33% 3.348 105.97% 61 3.401 3.408 0.007 100.21% 0.903 377.47% 62 3.401 3.487 0.086 102.53% 0.903 386.21% 71 3.401 3.537 0.137 104.02% 0.802 441.04% 72 3.401 3.404 0.004 100.11% 0.802 424.47% ARS EHD ARS value ARS − EHD (ARS/EHD) % TP ARS/TP (%) 11 10.618  10.996  0.378 103.56% 6.025 182.50% 12 8.169 8.362 0.192 102.35% 6.025 138.78% 21 4.861 5.498 0.636 113.09% 1.682 326.79% 22 3.761 4.178 0.418 111.10% 1.682 248.36% 31 3.679 3.851 0.172 104.67% 1.212 317.83% 32 3.465 3.467 0.002 100.06% 1.212 286.15% 41 3.519 3.547 0.028 100.81% 0.488 726.34% 42 3.635 3.702 0.067 101.84% 0.488 757.93% 51 3.846 3.849 0.002 100.06% 3.348 114.96% 52 4.514 5.198 0.684 115.15% 3.348 155.25% 61 4.767 4.852 0.086 101.79% 0.903 537.47% 62 4.832 4.992 0.160 103.32% 0.903 552.99% 71 5.087 5.799 0.712 114.00% 0.802 723.05% 72 6.367 6.646 0.280 104.39% 0.802 828.65%

The results of the equations of the seventh embodiment based on Table 15 and Table 16 are listed in the following table:

Values related to the inflection points of the eighth embodiment (Reference wavelength: 555 nm) HIF111 5.7971 HIF111/HOI 0.7729 SGI111 −1.1533 |SGI111|/(|SGI111| + TP1) 0.1607 HIF121 4.2725 HIF121/HOI 0.5697 SGI121 −0.8143 |SGI121|/(|SGI121| + TP1) 0.1191 HIF311 3.4672 HIF311/HOI 0.4623 SGI311 0.8644 |SGI311|/(|SGI311| + TP3) 0.4164 HIF321 1.6633 HIF321/HOI 0.2218 SGI321 0.0549 |SGI321|/(|SGI321| + TP3) 0.0433 HIF411 1.7967 HIF411/HOI 0.2396 SGI411 −0.2102 |SGI411|/(|SGI411| + TP4) 0.3009 HIF421 1.2296 HIF421/HOI 0.1639 SGI421 −0.0678 |SGI421|/(|SGI421| + TP4) 0.1218 HIF511 1.7386 HIF511/HOI 0.2318 SGI511 0.0615 |SGI511|/(|SGI511| + TP5) 0.0180 HIF512 3.5193 HIF512/HOI 0.4692 SGI512 0.0971 |SGI512|/(|SGI512| + TP5) 0.0282 HIF611 4.4931 HIF611/HOI 0.5991 SGI611 −0.5031 |SGI611|/(|SGI611| + TP6) 0.3578 HIF621 3.9380 HIF621/HOI 0.5251 SGI621 −0.8862 |SGI621|/(|SGI621| + TP6) 0.4954 HIF721 1.7203 HIF721/HOI 0.2294 SGI721 0.0807 |SGI721|/(|SGI721| + TP7) 0.0915 HIF722 6.3001 HIF722/HOI 0.8400 SGI722 −0.9321 |SGI722|/(|SGI722| + TP7) 0.5375

It must be pointed out that the embodiments described above are only some embodiments of the present invention. All equivalent structures which employ the concepts disclosed in this specification and the appended claims should fall within the scope of the present invention. 

What is claimed is:
 1. An optical image capturing system, in order along an optical axis from an object side to an image side, comprising: a first lens having positive refractive power; a second lens having refractive power; a third lens having refractive power; a fourth lens having refractive power; a fifth lens having refractive power; a sixth lens having refractive power; a seventh lens having refractive power; and an image plane; wherein the optical image capturing system consists of the seven lenses with refractive power; a maximum height for image formation perpendicular to the optical axis on the image plane is denoted as HOI; at least one lens among the second lens to the seventh lens has positive refractive power; the seventh lens has an object-side surface, which faces the object side, and an image-side surface, which faces the image side, and the object-side surface and the image-side surface of the seventh lens are aspheric surfaces; wherein the optical image capturing system satisfies: 1.2≦f/HEP≦10.0; 0<InTL/HOS<0.9; and 0.9≦2(ARE/HEP)≦1.5; where f1, f2, f3, f4, f5, f6, and f7 are focal lengths of the first lens to the seventh lens, respectively; f is a focal length of the optical image capturing system; HEP is an entrance pupil diameter of the optical image capturing system; HOS is a distance in parallel with the optical axis from an object-side surface of the first lens to the image plane; InTL is a distance in parallel with the optical axis from the object-side surface of the first lens to the image-side surface of the seventh lens; for any surface of any lens, ARE is a profile curve length measured from a start point where the optical axis passes therethrough, along a surface profile thereof, and finally to a coordinate point of a perpendicular distance where is a half of the entrance pupil diameter away from the optical axis.
 2. The optical image capturing system of claim 1, wherein the optical image capturing system further satisfies: PLTA≦200 μm; PSTA≦200 μm; NLTA≦200 μm; NSTA≦200 μm; SLTA≦200 μm; SSTA≦200 μm; and |TDT|<250%; where TDT is a TV distortion; HOI is a maximum height for image formation perpendicular to the optical axis on the image plane; PLTA is a transverse aberration at 0.7 HOI on the image plane in the positive direction of a tangential fan of the optical image capturing system after a longest operation wavelength of visible light passing through an edge of the aperture; PSTA is a transverse aberration at 0.7 HOI on the image plane in the positive direction of the tangential fan after a shortest operation wavelength of visible light passing through the edge of the aperture; NLTA is a transverse aberration at 0.7 HOI on the image plane in the negative direction of the tangential fan after the longest operation wavelength of visible light passing through the edge of the aperture; NSTA is a transverse aberration at 0.7 HOI on the image plane in the negative direction of the tangential fan after the shortest operation wavelength of visible light passing through the edge of the aperture; SLTA is a transverse aberration at 0.7 HOI on the image plane of a sagittal fan of the optical image capturing system after the longest operation wavelength of visible light passing through the edge of the aperture; SSTA is a transverse aberration at 0.7 HOI on the image plane of a sagittal fan after the shortest operation wavelength of visible light passing through the edge of the aperture.
 3. The optical image capturing system of claim 1, wherein the optical image capturing system further satisfies: 0.9≦ARS/EHD≦2.0; where, for any surface of any lens, EHD is a maximum effective half diameter thereof, ARS is a profile curve length measured from a start point where the optical axis passes therethrough, along a surface profile thereof, and finally to an end point of the maximum effective half diameter thereof.
 4. The optical image capturing system of claim 1, wherein the optical image capturing system further satisfies: 0 mm<HOS≦50 mm.
 5. The optical image capturing system of claim 1, wherein the optical image capturing system further satisfies: 0 deg<HAF≦100 deg; where HAF is a half of a view angle of the optical image capturing system.
 6. The optical image capturing system of claim 1, wherein the optical image capturing system further satisfies: 0.05≦ARE71/TP7≦25; and 0.05≦ARE72/TP7≦25; where ARE71 is a profile curve length measured from a start point where the optical axis passes the object-side surface of the seventh lens, along a surface profile of the object-side surface of the seventh lens, and finally to a coordinate point of a perpendicular distance where is a half of the entrance pupil diameter away from the optical axis; ARE72 is a profile curve length measured from a start point where the optical axis passes the image-side surface of the seventh lens, along a surface profile of the image-side surface of the seventh lens, and finally to a coordinate point of a perpendicular distance where is a half of the entrance pupil diameter away from the optical axis; TP7 is a thickness of the seventh lens on the optical axis.
 7. The optical image capturing system of claim 1, wherein the optical image capturing system further satisfies: 0.05≦ARE61/TP6≦25; and 0.05≦ARE62/TP6≦25; where ARE61 is a profile curve length measured from a start point where the optical axis passes the object-side surface of the sixth lens, along a surface profile of the object-side surface of the sixth lens, and finally to a coordinate point of a perpendicular distance where is a half of the entrance pupil diameter away from the optical axis; ARE62 is a profile curve length measured from a start point where the optical axis passes the image-side surface of the sixth lens, along a surface profile of the image-side surface of the sixth lens, and finally to a coordinate point of a perpendicular distance where is a half of the entrance pupil diameter away from the optical axis; TP6 is a thickness of the sixth lens on the optical axis.
 8. The optical image capturing system of claim 1, wherein the first lens has positive refractive power, and the second lens has negative refractive power.
 9. The optical image capturing system of claim 1, further comprising an aperture, wherein the optical image capturing system further satisfies: 0.2≦InS/HOS≦1.1; where InS is a distance in parallel with the optical axis between the aperture and the image plane.
 10. An optical image capturing system, in order along an optical axis from an object side to an image side, comprising: a first lens having positive refractive power; a second lens having refractive power; a third lens having refractive power; a fourth lens having refractive power; a fifth lens having refractive power; a sixth lens having refractive power; a seventh lens having refractive power; and an image plane; wherein the optical image capturing system consists of the seven lenses with refractive power; at least a surface of each of at least two lenses among the first lens to the seventh lens has at least an inflection point; at least one lens between the second lens and the seventh lens has positive refractive power; wherein the optical image capturing system satisfies: 1.2≦f/HEP≦10.0; 0<InTL/HOS<0.9; and 0.9≦2(ARE/HEP)≦1.5; where f1, f2, f3, f4, f5, f6, and f7 are focal lengths of the first lens to the seventh lens, respectively; f is a focal length of the optical image capturing system; HEP is an entrance pupil diameter of the optical image capturing system; HOS is a distance in parallel with the optical axis between an object-side surface, which face the object side, of the first lens and the image plane; InTL is a distance from the object-side surface of the first lens to the image-side surface of the seventh lens; for any surface of any lens, ARE is a profile curve length measured from a start point where the optical axis passes therethrough, along a surface profile thereof, and finally to a coordinate point of a perpendicular distance where is a half of the entrance pupil diameter away from the optical axis.
 11. The optical image capturing system of claim 10, wherein the optical image capturing system further satisfies: 0.9≦ARS/EHD≦2.0; where, for any surface of any lens, EHD is a maximum effective half diameter thereof, ARS is a profile curve length measured from a start point where the optical axis passes therethrough, along a surface profile thereof, and finally to an end point of the maximum effective half diameter thereof.
 12. The optical image capturing system of claim 10, wherein at least a surface of at least one lens among the first lens to the seventh lens has at least two inflection points thereon.
 13. The optical image capturing system of claim 10, wherein the optical image capturing system further satisfies: PLTA≦200 μm; PSTA≦200 μm; NLTA≦200 μm; NSTA≦200 μm; SLTA≦200 μm; SSTA≦200 μm; and HOI>3.0 mm where HOI is a maximum height for image formation perpendicular to the optical axis on the image plane; PLTA is a transverse aberration at 0.7 HOI on the image plane in the positive direction of a tangential fan of the optical image capturing system after a longest operation wavelength of visible light passing through an edge of the aperture; PSTA is a transverse aberration at 0.7 HOI on the image plane in the positive direction of the tangential fan after a shortest operation wavelength of visible light passing through the edge of the aperture; NLTA is a transverse aberration at 0.7 HOI on the image plane in the negative direction of the tangential fan after the longest operation wavelength of visible light passing through the edge of the aperture; NSTA is a transverse aberration at 0.7 HOI on the image plane in the negative direction of the tangential fan after the shortest operation wavelength of visible light passing through the edge of the aperture; SLTA is a transverse aberration at 0.7 HOI on the image plane of a sagittal fan of the optical image capturing system after the longest operation wavelength of visible light passing through the edge of the aperture; SSTA is a transverse aberration at 0.7 HOI on the image plane of a sagittal fan after the shortest operation wavelength of visible light passing through the edge of the aperture.
 14. The optical image capturing system of claim 10, wherein at least one lens among the first lens, the second lens, the third lens, the fourth lens, the fifth lens, the sixth lens, and the seventh lens is a filter, which is capable of filtering out light of wavelengths shorter than 500 nm.
 15. The optical image capturing system of claim 10, wherein the optical image capturing system further satisfies: 0<IN12/f≦3.0; where IN12 is a distance on the optical axis between the first lens and the second lens.
 16. The optical image capturing system of claim 10, wherein the optical image capturing system further satisfies: 0<IN67/f≦0.8; where IN67 is a distance on the optical axis between the sixth lens and the seventh lens.
 17. The optical image capturing system of claim 10, wherein the optical image capturing system further satisfies: 0.1≦(TP7+IN67)/TP6≦10; where IN67 is a distance on the optical axis between the sixth lens and the seventh lens; TP6 is a thickness of the sixth lens on the optical axis; TP7 is a thickness of the seventh lens on the optical axis.
 18. The optical image capturing system of claim 10, wherein the optical image capturing system further satisfies: 0.1≦(TP1+IN12)/TP2≦10; where IN12 is a distance on the optical axis between the first lens and the second lens; TP1 is a thickness of the first lens on the optical axis; TP2 is a thickness of the second lens on the optical axis.
 19. The optical image capturing system of claim 10, wherein the optical image capturing system further satisfies: 0<TP4/(IN34+TP4+IN45)<1; where IN34 is a distance on the optical axis between the third lens and the fourth lens; IN45 is a distance on the optical axis between the fourth lens and the fifth lens; TP4 is a thickness of the fourth lens on the optical axis.
 20. An optical image capturing system, in order along an optical axis from an object side to an image side, comprising: a first lens having positive refractive power; a second lens having refractive power; a third lens having refractive power; a fourth lens having refractive power; a fifth lens having refractive power; a sixth lens having refractive power; a seventh lens having refractive power; and an image plane; wherein the optical image capturing system consists of the seven lenses having refractive power; a maximum height for image formation perpendicular to the optical axis on the image plane is denoted as HOI; at least a surface of each of at least three lenses among the first lens to the sixth lens has at least an inflection point thereon; both an object-side surface, which faces the object side, and an image-side surface, which faces the image side, of at least one lens among the first lens to the seventh lens are aspheric surfaces; wherein the optical image capturing system satisfies: 1.2≦f/HEP≦3.5; 0.4≦|tan(HAF)|≦1.5; 0<InTL/HOS<0.9; and 0.9≦2(ARE/HEP)≦1.5; where f1, f2, f3, f4, f5, f6, and f7 are focal lengths of the first lens to the seventh lens, respectively; f is a focal length of the optical image capturing system; HEP is an entrance pupil diameter of the optical image capturing system; HAF is a half of a view angle of the optical image capturing system; HOS is a distance in parallel with the optical axis between an object-side surface, which face the object side, of the first lens and the image plane; InTL is a distance from the object-side surface of the first lens to the image-side surface of the seventh lens; for any surface of any lens, ARE is a profile curve length measured from a start point where the optical axis passes therethrough, along a surface profile thereof, and finally to a coordinate point of a perpendicular distance where is a half of the entrance pupil diameter away from the optical axis.
 21. The optical image capturing system of claim 20, wherein the optical image capturing system further satisfies: 0.9≦ARS/EHD≦2.0; where, for any surface of any lens, EHD is a maximum effective half diameter thereof, ARS is a profile curve length measured from a start point where the optical axis passes therethrough, along a surface profile thereof, and finally to an end point of the maximum effective half diameter thereof.
 22. The optical image capturing system of claim 20, wherein the optical image capturing system further satisfies: 0 mm<HOS≦50 mm.
 23. The optical image capturing system of claim 20, wherein the optical image capturing system further satisfies: 0.05≦ARE71/TP7≦25; and 0.05≦ARE72/TP7≦25; where ARE71 is a profile curve length measured from a start point where the optical axis passes the object-side surface of the seventh lens, along a surface profile of the object-side surface of the seventh lens, and finally to a coordinate point of a perpendicular distance where is a half of the entrance pupil diameter away from the optical axis; ARE72 is a profile curve length measured from a start point where the optical axis passes the image-side surface of the seventh lens, along a surface profile of the image-side surface of the seventh lens, and finally to a coordinate point of a perpendicular distance where is a half of the entrance pupil diameter away from the optical axis; TP7 is a thickness of the seventh lens on the optical axis.
 24. The optical image capturing system of claim 20, wherein the optical image capturing system further satisfies: 0.05≦ARE61/TP6≦25; and 0.05≦ARE62/TP6≦25; where ARE61 is a profile curve length measured from a start point where the optical axis passes the object-side surface of the sixth lens, along a surface profile of the object-side surface of the sixth lens, and finally to a coordinate point of a perpendicular distance where is a half of the entrance pupil diameter away from the optical axis; ARE62 is a profile curve length measured from a start point where the optical axis passes the image-side surface of the sixth lens, along a surface profile of the image-side surface of the sixth lens, and finally to a coordinate point of a perpendicular distance where is a half of the entrance pupil diameter away from the optical axis; TP6 is a thickness of the sixth lens on the optical axis.
 25. The optical image capturing system of claim 20, further comprising an aperture an image sensor, and a driving module, wherein the image sensor is disposed on the image plane; the driving module is coupled with the lenses to move the lenses; the optical image capturing system further satisfies: 0.2≦InS/HOS≦1.1; where InS is a distance in parallel with the optical axis between the aperture and the image plane. 